K |
Name | Schema Table | Database | Description | Type | Length | Unit | Default Value | Unified Content Descriptor |
K |
twomass |
SIXDF |
K magnitude (corrected) used for K selection |
real |
4 |
mag |
|
|
k1 |
catwise_2020, catwise_prelim |
WISE |
W1 photometry usage code (0: neither the ascending nor the descending scan provided a solution; 1: only the ascending scan provided a solution; 2: only the descending scan provided a solution; 3: both scans provided solutions which were combined in the relevant way) |
int |
4 |
|
|
|
k2 |
catwise_2020, catwise_prelim |
WISE |
W2 photometry usage code (0: neither the ascending nor the descending scan provided a solution; 1: only the ascending scan provided a solution; 2: only the descending scan provided a solution; 3: both scans provided solutions which were combined in the relevant way) |
int |
4 |
|
|
|
k_2mrat |
twomass_scn |
TWOMASS |
Ks-band average 2nd image moment ratio. |
real |
4 |
|
|
stat.fit.param |
k_2mrat |
twomass_sixx2_scn |
TWOMASS |
K band average 2nd image moment ratio for scan |
real |
4 |
|
|
|
k_5sig_ba |
twomass_xsc |
TWOMASS |
K minor/major axis ratio fit to the 5-sigma isophote. |
real |
4 |
|
|
phys.size.axisRatio |
k_5sig_phi |
twomass_xsc |
TWOMASS |
K angle to 5-sigma major axis (E of N). |
smallint |
2 |
degrees |
|
stat.error |
k_5surf |
twomass_xsc |
TWOMASS |
K central surface brightness (r<=5). |
real |
4 |
mag |
|
phot.mag.sb |
k_ba |
twomass_sixx2_xsc |
TWOMASS |
K minor/major axis ratio fit to the 3-sigma isophote |
real |
4 |
|
|
|
k_ba |
twomass_xsc |
TWOMASS |
K minor/major axis ratio fit to the 3-sigma isophote. |
real |
4 |
|
|
phys.size.axisRatio |
k_back |
twomass_xsc |
TWOMASS |
K coadd median background. |
real |
4 |
|
|
meta.code |
k_bisym_chi |
twomass_xsc |
TWOMASS |
K bi-symmetric cross-correlation chi. |
real |
4 |
|
|
stat.fit.param |
k_bisym_rat |
twomass_xsc |
TWOMASS |
K bi-symmetric flux ratio. |
real |
4 |
|
|
phot.flux;arith.ratio |
k_bndg_amp |
twomass_xsc |
TWOMASS |
K banding maximum FT amplitude on this side of coadd. |
real |
4 |
DN |
|
stat.fit.param |
k_bndg_per |
twomass_xsc |
TWOMASS |
K banding Fourier Transf. period on this side of coadd. |
int |
4 |
arcsec |
|
stat.fit.param |
k_chif_ellf |
twomass_xsc |
TWOMASS |
K % chi-fraction for elliptical fit to 3-sig isophote. |
real |
4 |
|
|
stat.fit.param |
k_cmsig |
twomass_psc |
TWOMASS |
Corrected photometric uncertainty for the default Ks-band magnitude. |
real |
4 |
mag |
Ks-band |
phot.flux |
k_con_indx |
twomass_xsc |
TWOMASS |
K concentration index r_75%/r_25%. |
real |
4 |
|
|
phys.size;arith.ratio |
k_d_area |
twomass_xsc |
TWOMASS |
K 5-sigma to 3-sigma differential area. |
smallint |
2 |
|
|
stat.fit.residual |
k_flg_10 |
twomass_xsc |
TWOMASS |
K confusion flag for 10 arcsec circular ap. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_15 |
twomass_xsc |
TWOMASS |
K confusion flag for 15 arcsec circular ap. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_20 |
twomass_xsc |
TWOMASS |
K confusion flag for 20 arcsec circular ap. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_25 |
twomass_xsc |
TWOMASS |
K confusion flag for 25 arcsec circular ap. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_30 |
twomass_xsc |
TWOMASS |
K confusion flag for 30 arcsec circular ap. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_40 |
twomass_xsc |
TWOMASS |
K confusion flag for 40 arcsec circular ap. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_5 |
twomass_xsc |
TWOMASS |
K confusion flag for 5 arcsec circular ap. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_50 |
twomass_xsc |
TWOMASS |
K confusion flag for 50 arcsec circular ap. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_60 |
twomass_xsc |
TWOMASS |
K confusion flag for 60 arcsec circular ap. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_7 |
twomass_sixx2_xsc |
TWOMASS |
K confusion flag for 7 arcsec circular ap. mag |
smallint |
2 |
|
|
|
k_flg_7 |
twomass_xsc |
TWOMASS |
K confusion flag for 7 arcsec circular ap. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_70 |
twomass_xsc |
TWOMASS |
K confusion flag for 70 arcsec circular ap. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_c |
twomass_xsc |
TWOMASS |
K confusion flag for Kron circular mag. |
smallint |
2 |
|
|
meta.code |
k_flg_e |
twomass_xsc |
TWOMASS |
K confusion flag for Kron elliptical mag. |
smallint |
2 |
|
|
meta.code |
k_flg_fc |
twomass_xsc |
TWOMASS |
K confusion flag for fiducial Kron circ. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_fe |
twomass_xsc |
TWOMASS |
K confusion flag for fiducial Kron ell. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_i20c |
twomass_xsc |
TWOMASS |
K confusion flag for 20mag/sq." iso. circ. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_i20e |
twomass_xsc |
TWOMASS |
K confusion flag for 20mag/sq." iso. ell. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_i21c |
twomass_xsc |
TWOMASS |
K confusion flag for 21mag/sq." iso. circ. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_i21e |
twomass_xsc |
TWOMASS |
K confusion flag for 21mag/sq." iso. ell. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_j21fc |
twomass_xsc |
TWOMASS |
K confusion flag for 21mag/sq." iso. fid. circ. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_j21fe |
twomass_xsc |
TWOMASS |
K confusion flag for 21mag/sq." iso. fid. ell. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_k20fc |
twomass_xsc |
TWOMASS |
K confusion flag for 20mag/sq." iso. fid. circ. mag. |
smallint |
2 |
|
|
meta.code |
k_flg_k20fe |
twomass_sixx2_xsc |
TWOMASS |
K confusion flag for 20mag/sq.″ iso. fid. ell. mag |
smallint |
2 |
|
|
|
k_flg_k20fe |
twomass_xsc |
TWOMASS |
K confusion flag for 20mag/sq." iso. fid. ell. mag. |
smallint |
2 |
|
|
meta.code |
k_m |
twomass_psc |
TWOMASS |
Default Ks-band magnitude |
real |
4 |
mag |
|
phot.flux |
k_m |
twomass_sixx2_psc |
TWOMASS |
K selected "default" magnitude |
real |
4 |
mag |
|
|
k_m_10 |
twomass_xsc |
TWOMASS |
K 10 arcsec radius circular aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_15 |
twomass_xsc |
TWOMASS |
K 15 arcsec radius circular aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_20 |
twomass_xsc |
TWOMASS |
K 20 arcsec radius circular aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_25 |
twomass_xsc |
TWOMASS |
K 25 arcsec radius circular aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_2mass |
allwise_sc |
WISE |
2MASS Ks-band magnitude of the associated 2MASS PSC source. This column is "null" if there is no associated 2MASS PSC source or if the 2MASS PSC Ks-band magnitude entry is "null". |
float |
8 |
mag |
|
|
k_m_2mass |
wise_allskysc |
WISE |
2MASS Ks-band magnitude or magnitude upper limit of the associated 2MASS PSC source. This column is default if there is no associated 2MASS PSC source or if the 2MASS PSC Ks-band magnitude entry is default. |
real |
4 |
mag |
-0.9999995e9 |
|
k_m_2mass |
wise_prelimsc |
WISE |
2MASS Ks-band magnitude or magnitude upper limit of the associated 2MASS PSC source This column is default if there is no associated 2MASS PSC source or if the 2MASS PSC Ks-band magnitude entry is default |
real |
4 |
mag |
-0.9999995e9 |
|
k_m_30 |
twomass_xsc |
TWOMASS |
K 30 arcsec radius circular aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_40 |
twomass_xsc |
TWOMASS |
K 40 arcsec radius circular aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_5 |
twomass_xsc |
TWOMASS |
K 5 arcsec radius circular aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_50 |
twomass_xsc |
TWOMASS |
K 50 arcsec radius circular aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_60 |
twomass_xsc |
TWOMASS |
K 60 arcsec radius circular aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_7 |
twomass_sixx2_xsc |
TWOMASS |
K 7 arcsec radius circular aperture magnitude |
real |
4 |
mag |
|
|
k_m_7 |
twomass_xsc |
TWOMASS |
K 7 arcsec radius circular aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_70 |
twomass_xsc |
TWOMASS |
K 70 arcsec radius circular aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_c |
twomass_xsc |
TWOMASS |
K Kron circular aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_e |
twomass_xsc |
TWOMASS |
K Kron elliptical aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_ext |
twomass_sixx2_xsc |
TWOMASS |
K mag from fit extrapolation |
real |
4 |
mag |
|
|
k_m_ext |
twomass_xsc |
TWOMASS |
K mag from fit extrapolation. |
real |
4 |
mag |
|
phot.flux |
k_m_fc |
twomass_xsc |
TWOMASS |
K fiducial Kron circular magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_fe |
twomass_xsc |
TWOMASS |
K fiducial Kron ell. mag aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_i20c |
twomass_xsc |
TWOMASS |
K 20mag/sq." isophotal circular ap. magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_i20e |
twomass_xsc |
TWOMASS |
K 20mag/sq." isophotal elliptical ap. magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_i21c |
twomass_xsc |
TWOMASS |
K 21mag/sq." isophotal circular ap. magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_i21e |
twomass_xsc |
TWOMASS |
K 21mag/sq." isophotal elliptical ap. magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_j21fc |
twomass_xsc |
TWOMASS |
K 21mag/sq." isophotal fiducial circ. ap. mag. |
real |
4 |
mag |
|
phot.flux |
k_m_j21fe |
twomass_xsc |
TWOMASS |
K 21mag/sq." isophotal fiducial ell. ap. magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_k20fc |
twomass_xsc |
TWOMASS |
K 20mag/sq." isophotal fiducial circ. ap. mag. |
real |
4 |
mag |
|
phot.flux |
K_M_K20FE |
twomass |
SIXDF |
K 20mag/sq." isophotal fiducial ell. ap. magnitude |
real |
4 |
mag |
|
|
k_m_k20fe |
twomass_sixx2_xsc |
TWOMASS |
K 20mag/sq.″ isophotal fiducial ell. ap. magnitude |
real |
4 |
mag |
|
|
k_m_k20fe |
twomass_xsc |
TWOMASS |
K 20mag/sq." isophotal fiducial ell. ap. magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_stdap |
twomass_psc |
TWOMASS |
Ks-band "standard" aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_m_sys |
twomass_xsc |
TWOMASS |
K system photometry magnitude. |
real |
4 |
mag |
|
phot.flux |
k_mnsurfb_eff |
twomass_xsc |
TWOMASS |
K mean surface brightness at the half-light radius. |
real |
4 |
mag |
|
phot.mag.sb |
k_msig |
twomass_sixx2_psc |
TWOMASS |
K "default" mag uncertainty |
real |
4 |
mag |
|
|
k_msig_10 |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 10 arcsec circular ap. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_15 |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 15 arcsec circular ap. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_20 |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 20 arcsec circular ap. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_25 |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 25 arcsec circular ap. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_2mass |
allwise_sc |
WISE |
2MASS Ks-band corrected photometric uncertainty of the associated 2MASS PSC source. This column is "null" if there is no associated 2MASS PSC source or if the 2MASS PSC Ks-band uncertainty entry is "null". |
float |
8 |
mag |
|
|
k_msig_2mass |
wise_allskysc |
WISE |
2MASS Ks-band corrected photometric uncertainty of the associated 2MASS PSC source. This column is default if there is no associated 2MASS PSC source or if the 2MASS PSC Ks-band uncertainty entry is default. |
real |
4 |
mag |
-0.9999995e9 |
|
k_msig_2mass |
wise_prelimsc |
WISE |
2MASS Ks-band corrected photometric uncertainty of the associated 2MASS PSC source This column is default if there is no associated 2MASS PSC source or if the 2MASS PSC Ks-band uncertainty entry is default |
real |
4 |
mag |
-0.9999995e9 |
|
k_msig_30 |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 30 arcsec circular ap. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_40 |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 40 arcsec circular ap. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_5 |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 5 arcsec circular ap. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_50 |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 50 arcsec circular ap. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_60 |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 60 arcsec circular ap. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_7 |
twomass_sixx2_xsc |
TWOMASS |
K 1-sigma uncertainty in 7 arcsec circular ap. mag |
real |
4 |
mag |
|
|
k_msig_7 |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 7 arcsec circular ap. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_70 |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 70 arcsec circular ap. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_c |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in Kron circular mag. |
real |
4 |
mag |
|
stat.error |
k_msig_e |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in Kron elliptical mag. |
real |
4 |
mag |
|
stat.error |
k_msig_ext |
twomass_sixx2_xsc |
TWOMASS |
K 1-sigma uncertainty in mag from fit extrapolation |
real |
4 |
mag |
|
|
k_msig_ext |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in mag from fit extrapolation. |
real |
4 |
mag |
|
stat.error |
k_msig_fc |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in fiducial Kron circ. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_fe |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in fiducial Kron ell. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_i20c |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 20mag/sq." iso. circ. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_i20e |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 20mag/sq." iso. ell. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_i21c |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 21mag/sq." iso. circ. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_i21e |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 21mag/sq." iso. ell. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_j21fc |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 21mag/sq." iso.fid.circ.mag. |
real |
4 |
mag |
|
stat.error |
k_msig_j21fe |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 21mag/sq." iso.fid.ell.mag. |
real |
4 |
mag |
|
stat.error |
k_msig_k20fc |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 20mag/sq." iso.fid.circ. mag. |
real |
4 |
mag |
|
stat.error |
k_msig_k20fe |
twomass_sixx2_xsc |
TWOMASS |
K 1-sigma uncertainty in 20mag/sq.″ iso.fid.ell.mag |
real |
4 |
mag |
|
|
k_msig_k20fe |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in 20mag/sq." iso.fid.ell.mag. |
real |
4 |
mag |
|
stat.error |
k_msig_stdap |
twomass_psc |
TWOMASS |
Uncertainty in the Ks-band standard aperture magnitude. |
real |
4 |
mag |
|
phot.flux |
k_msig_sys |
twomass_xsc |
TWOMASS |
K 1-sigma uncertainty in system photometry mag. |
real |
4 |
mag |
|
stat.error |
k_msigcom |
twomass_psc |
TWOMASS |
Combined, or total photometric uncertainty for the default Ks-band magnitude. |
real |
4 |
mag |
Ks-band |
phot.flux |
k_msigcom |
twomass_sixx2_psc |
TWOMASS |
combined (total) K band photometric uncertainty |
real |
4 |
mag |
|
|
k_msnr10 |
twomass_scn |
TWOMASS |
The estimated Ks-band magnitude at which SNR=10 is achieved for this scan. |
real |
4 |
mag |
|
phot.flux |
k_msnr10 |
twomass_sixx2_scn |
TWOMASS |
K mag at which SNR=10 is achieved, from k_psp and k_zp_ap |
real |
4 |
mag |
|
|
k_n_snr10 |
twomass_scn |
TWOMASS |
Number of point sources at Ks-band with SNR>10 (instrumental mag <=14.3) |
int |
4 |
|
|
meta.number |
k_n_snr10 |
twomass_sixx2_scn |
TWOMASS |
number of K point sources with SNR>10 (instrumental m<=14.3) |
int |
4 |
|
|
|
k_pchi |
twomass_xsc |
TWOMASS |
K chi^2 of fit to rad. profile (LCSB: alpha scale len). |
real |
4 |
|
|
stat.fit.param |
k_peak |
twomass_xsc |
TWOMASS |
K peak pixel brightness. |
real |
4 |
mag |
|
phot.mag.sb |
k_perc_darea |
twomass_xsc |
TWOMASS |
K 5-sigma to 3-sigma percent area change. |
smallint |
2 |
|
|
FIT_PARAM |
k_phi |
twomass_sixx2_xsc |
TWOMASS |
K angle to 3-sigma major axis (E of N) |
smallint |
2 |
deg |
|
|
k_phi |
twomass_xsc |
TWOMASS |
K angle to 3-sigma major axis (E of N). |
smallint |
2 |
degrees |
|
pos.posAng |
k_psfchi |
twomass_psc |
TWOMASS |
Reduced chi-squared goodness-of-fit value for the Ks-band profile-fit photometry made on the 1.3 s "Read_2" exposures. |
real |
4 |
|
|
stat.fit.param |
k_psp |
twomass_scn |
TWOMASS |
Ks-band photometric sensitivity paramater (PSP). |
real |
4 |
|
|
instr.sensitivity |
k_psp |
twomass_sixx2_scn |
TWOMASS |
K photometric sensitivity param: k_shape_avg*(k_fbg_avg^.29) |
real |
4 |
|
|
|
k_pts_noise |
twomass_scn |
TWOMASS |
Base-10 logarithm of the mode of the noise distribution for all point source detections in the scan, where the noise is estimated from the measured Ks-band photometric errors and is expressed in units of mJy. |
real |
4 |
|
|
instr.det.noise |
k_pts_noise |
twomass_sixx2_scn |
TWOMASS |
log10 of K band modal point src noise estimate |
real |
4 |
logmJy |
|
|
k_r_c |
twomass_xsc |
TWOMASS |
K Kron circular aperture radius. |
real |
4 |
arcsec |
|
phys.angSize;src |
k_r_e |
twomass_xsc |
TWOMASS |
K Kron elliptical aperture semi-major axis. |
real |
4 |
arcsec |
|
phys.angSize;src |
k_r_eff |
twomass_xsc |
TWOMASS |
K half-light (integrated half-flux point) radius. |
real |
4 |
arcsec |
|
phys.angSize;src |
k_r_i20c |
twomass_xsc |
TWOMASS |
K 20mag/sq." isophotal circular aperture radius. |
real |
4 |
arcsec |
|
phys.angSize;src |
k_r_i20e |
twomass_xsc |
TWOMASS |
K 20mag/sq." isophotal elliptical ap. semi-major axis. |
real |
4 |
arcsec |
|
phys.angSize;src |
k_r_i21c |
twomass_xsc |
TWOMASS |
K 21mag/sq." isophotal circular aperture radius. |
real |
4 |
arcsec |
|
phys.angSize;src |
k_r_i21e |
twomass_xsc |
TWOMASS |
K 21mag/sq." isophotal elliptical ap. semi-major axis. |
real |
4 |
arcsec |
|
phys.angSize;src |
k_resid_ann |
twomass_xsc |
TWOMASS |
K residual annulus background median. |
real |
4 |
DN |
|
meta.code |
k_sc_1mm |
twomass_xsc |
TWOMASS |
K 1st moment (score) (LCSB: super blk 2,4,8 SNR). |
real |
4 |
|
|
meta.code |
k_sc_2mm |
twomass_xsc |
TWOMASS |
K 2nd moment (score) (LCSB: SNRMAX - super SNR max). |
real |
4 |
|
|
meta.code |
k_sc_msh |
twomass_xsc |
TWOMASS |
K median shape score. |
real |
4 |
|
|
meta.code |
k_sc_mxdn |
twomass_xsc |
TWOMASS |
K mxdn (score) (LCSB: BSNR - block/smoothed SNR). |
real |
4 |
|
|
meta.code |
k_sc_r1 |
twomass_xsc |
TWOMASS |
K r1 (score). |
real |
4 |
|
|
meta.code |
k_sc_r23 |
twomass_xsc |
TWOMASS |
K r23 (score) (LCSB: TSNR - integrated SNR for r=15). |
real |
4 |
|
|
meta.code |
k_sc_sh |
twomass_xsc |
TWOMASS |
K shape (score). |
real |
4 |
|
|
meta.code |
k_sc_vint |
twomass_xsc |
TWOMASS |
K vint (score). |
real |
4 |
|
|
meta.code |
k_sc_wsh |
twomass_xsc |
TWOMASS |
K wsh (score) (LCSB: PSNR - peak raw SNR). |
real |
4 |
|
|
meta.code |
k_seetrack |
twomass_xsc |
TWOMASS |
K band seetracking score. |
real |
4 |
|
|
meta.code |
k_sh0 |
twomass_xsc |
TWOMASS |
K ridge shape (LCSB: BSNR limit). |
real |
4 |
|
|
FIT_PARAM |
k_shape_avg |
twomass_scn |
TWOMASS |
Ks-band average seeing shape for scan. |
real |
4 |
|
|
instr.obsty.seeing |
k_shape_avg |
twomass_sixx2_scn |
TWOMASS |
K band average seeing shape for scan |
real |
4 |
|
|
|
k_shape_rms |
twomass_scn |
TWOMASS |
RMS-error of Ks-band average seeing shape. |
real |
4 |
|
|
instr.obsty.seeing |
k_shape_rms |
twomass_sixx2_scn |
TWOMASS |
rms of K band avg seeing shape for scan |
real |
4 |
|
|
|
k_sig_sh0 |
twomass_xsc |
TWOMASS |
K ridge shape sigma (LCSB: B2SNR limit). |
real |
4 |
|
|
FIT_PARAM |
k_snr |
twomass_psc |
TWOMASS |
Ks-band "scan" signal-to-noise ratio. |
real |
4 |
mag |
|
instr.det.noise |
k_snr |
twomass_sixx2_psc |
TWOMASS |
K band "scan" signal-to-noise ratio |
real |
4 |
|
|
|
k_subst2 |
twomass_xsc |
TWOMASS |
K residual background #2 (score). |
real |
4 |
|
|
meta.code |
k_zp_ap |
twomass_scn |
TWOMASS |
Photometric zero-point for Ks-band aperture photometry. |
real |
4 |
mag |
|
phot.mag;arith.zp |
k_zp_ap |
twomass_sixx2_scn |
TWOMASS |
K band ap. calibration photometric zero-point for scan |
real |
4 |
mag |
|
|
k_zperr_ap |
twomass_scn |
TWOMASS |
RMS-error of zero-point for Ks-band aperture photometry |
real |
4 |
mag |
|
stat.error |
k_zperr_ap |
twomass_sixx2_scn |
TWOMASS |
K band ap. calibration rms error of zero-point for scan |
real |
4 |
mag |
|
|
ka |
catwise_2020, catwise_prelim |
WISE |
astrometry usage code (0: neither the ascending nor the descending scan provided a solution; 1: only the ascending scan provided a solution; 2: only the descending scan provided a solution; 3: both scans provided solutions which were combined in the relevant way) |
int |
4 |
|
|
|
KBESTR |
spectra |
SIXDF |
cross-correlation template |
int |
4 |
|
|
|
kCorr |
twompzPhotoz |
TWOMPZ |
K 20mag/sq." isophotal fiducial ell. ap. magnitude with Galactic dust correction {image primary HDU keyword: Kcorr} |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
kCorrErr |
twompzPhotoz |
TWOMPZ |
K 1-sigma uncertainty in 20mag/sq." aperture {image primary HDU keyword: k_msig_k20fe} |
real |
4 |
mag |
-0.9999995e9 |
|
KEXT |
twomass |
SIXDF |
KEXT magnitude |
real |
4 |
mag |
|
|
KEXT_K |
twomass |
SIXDF |
KEXT minus K (corrected) |
real |
4 |
mag |
|
|
kFi2 |
vvvVivaCatalogue |
VVVDR5 |
Even dispersion parameter of K_s pawprint data {catalogue TType keyword: Kfi2} |
float |
8 |
mag |
-9.999995e8 |
|
km |
catwise_2020, catwise_prelim |
WISE |
proper motion usage code (0: neither the ascending nor the descending scan provided a solution; 1: only the ascending scan provided a solution; 2: only the descending scan provided a solution; 3: both scans provided solutions which were combined in the relevant way) |
int |
4 |
|
|
|
Kmag |
mcps_lmcSource, mcps_smcSource |
MCPS |
The K' band magnitude (from 2MASS) (0.00 if star not detected.) |
real |
4 |
mag |
|
|
kMag |
ukirtFSstars |
VIDEOv20100513 |
K band total magnitude on the MKO(UFTI) system |
real |
4 |
mag |
|
phot.mag |
kMag |
ukirtFSstars |
VIKINGv20110714 |
K band total magnitude on the MKO(UFTI) system |
real |
4 |
mag |
|
phot.mag |
kMag |
ukirtFSstars |
VVVv20100531 |
K band total magnitude on the MKO(UFTI) system |
real |
4 |
mag |
|
phot.mag |
Kmag2MASS |
spitzer_smcSource |
SPITZER |
The 2MASS K band magnitude. |
real |
4 |
mag |
|
|
Kmag_2MASS |
ravedr5Source |
RAVE |
K selected default magnitude from 2MASS |
real |
4 |
mag |
magnitude |
phot.mag;em.IR.K |
Kmag_DENIS |
ravedr5Source |
RAVE |
K selected default magnitude |
real |
4 |
mag |
magnitude |
phot.mag;em.IR.K |
kMagErr |
ukirtFSstars |
VIDEOv20100513 |
K band magnitude error |
real |
4 |
mag |
|
stat.error |
kMagErr |
ukirtFSstars |
VIKINGv20110714 |
K band magnitude error |
real |
4 |
mag |
|
stat.error |
kMagErr |
ukirtFSstars |
VVVv20100531 |
K band magnitude error |
real |
4 |
mag |
|
stat.error |
kronFlux |
Detection |
PS1DR2 |
Kron (1980) flux. |
real |
4 |
Janskys |
-999 |
|
kronFlux |
sharksDetection |
SHARKSv20210222 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
sharksDetection |
SHARKSv20210421 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
ultravistaDetection |
ULTRAVISTADR4 |
flux within Kron radius circular aperture (SE: FLUX_AUTO) {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
ultravistaMapRemeasurement |
ULTRAVISTADR4 |
flux within Kron radius circular aperture (SE: FLUX_AUTO; CASU: default) {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSDR2 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
vhsDetection |
VHSDR3 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSDR4 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSDR5 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSDR6 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSv20120926 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSv20130417 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSv20140409 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSv20150108 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSv20160114 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSv20160507 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSv20170630 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSv20180419 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSv20201209 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSv20231101 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection |
VHSv20240731 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vhsDetection, vhsListRemeasurement |
VHSDR1 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
videoDetection |
VIDEODR2 |
flux within Kron radius circular aperture (SE: FLUX_AUTO) {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
videoDetection |
VIDEODR3 |
flux within Kron radius circular aperture (SE: FLUX_AUTO) {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
videoDetection |
VIDEODR4 |
flux within Kron radius circular aperture (SE: FLUX_AUTO) {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
videoDetection |
VIDEODR5 |
flux within Kron radius circular aperture (SE: FLUX_AUTO) {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
videoDetection |
VIDEOv20100513 |
flux within Kron radius circular aperture (SE: FLUX_AUTO) {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
videoDetection |
VIDEOv20111208 |
flux within Kron radius circular aperture (SE: FLUX_AUTO) {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
videoListRemeasurement |
VIDEOv20100513 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
vikingDetection |
VIKINGDR2 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
vikingDetection |
VIKINGDR3 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vikingDetection |
VIKINGDR4 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vikingDetection |
VIKINGv20111019 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
vikingDetection |
VIKINGv20130417 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vikingDetection |
VIKINGv20140402 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vikingDetection |
VIKINGv20150421 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vikingDetection |
VIKINGv20151230 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vikingDetection |
VIKINGv20160406 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vikingDetection |
VIKINGv20161202 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vikingDetection |
VIKINGv20170715 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vikingDetection, vikingListRemeasurement |
VIKINGv20110714 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
vikingMapRemeasurement |
VIKINGZYSELJv20160909 |
flux within Kron radius circular aperture (SE: FLUX_AUTO; CASU: default) {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
vikingMapRemeasurement |
VIKINGZYSELJv20170124 |
flux within Kron radius circular aperture (SE: FLUX_AUTO; CASU: default) {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
vmcDetection |
VMCDR1 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
vmcDetection |
VMCDR2 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCDR3 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCDR4 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCDR5 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20110909 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
vmcDetection |
VMCv20120126 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
vmcDetection |
VMCv20121128 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20130304 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20130805 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20140428 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20140903 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20150309 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20151218 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20160311 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20160822 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20170109 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20170411 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20171101 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20180702 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20181120 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20191212 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20210708 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20230816 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection |
VMCv20240226 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcDetection, vmcListRemeasurement |
VMCv20110816 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFlux |
vmcdeepDetection |
VMCDEEPv20230713 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vmcdeepDetection |
VMCDEEPv20240506 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vvvDetection |
VVVDR1 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vvvDetection |
VVVDR2 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vvvDetection, vvvDetectionPawPrints, vvvDetectionTiles |
VVVDR5 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count |
kronFlux |
vvvDetection, vvvListRemeasurement |
VVVv20100531 |
flux within circular aperture to k × r_k ; k = 2 {catalogue TType keyword: Kron_flux} |
real |
4 |
ADU |
|
phot.count;em.opt |
kronFluxErr |
Detection |
PS1DR2 |
Error on Kron (1980) flux. |
real |
4 |
Janskys |
-999 |
|
kronFluxErr |
sharksDetection |
SHARKSv20210222 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
sharksDetection |
SHARKSv20210421 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
ultravistaDetection |
ULTRAVISTADR4 |
error on Kron flux (SE: FLUXERR_AUTO) {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
ultravistaMapRemeasurement |
ULTRAVISTADR4 |
error on Kron flux (SE: FLUXERR_AUTO; CASU: default) {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSDR2 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSDR3 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSDR4 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSDR5 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSDR6 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSv20120926 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSv20130417 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSv20140409 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSv20150108 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSv20160114 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSv20160507 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSv20170630 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSv20180419 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSv20201209 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSv20231101 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection |
VHSv20240731 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vhsDetection, vhsListRemeasurement |
VHSDR1 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
videoDetection |
VIDEODR2 |
error on Kron flux (SE: FLUXERR_AUTO) {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
videoDetection |
VIDEODR3 |
error on Kron flux (SE: FLUXERR_AUTO) {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
videoDetection |
VIDEODR4 |
error on Kron flux (SE: FLUXERR_AUTO) {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
videoDetection |
VIDEODR5 |
error on Kron flux (SE: FLUXERR_AUTO) {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
videoDetection |
VIDEOv20100513 |
error on Kron flux (SE: FLUXERR_AUTO) {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
videoDetection |
VIDEOv20111208 |
error on Kron flux (SE: FLUXERR_AUTO) {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
videoListRemeasurement |
VIDEOv20100513 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingDetection |
VIKINGDR2 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingDetection |
VIKINGDR3 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingDetection |
VIKINGDR4 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingDetection |
VIKINGv20111019 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingDetection |
VIKINGv20130417 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingDetection |
VIKINGv20140402 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingDetection |
VIKINGv20150421 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingDetection |
VIKINGv20151230 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingDetection |
VIKINGv20160406 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingDetection |
VIKINGv20161202 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingDetection |
VIKINGv20170715 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingDetection, vikingListRemeasurement |
VIKINGv20110714 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingMapRemeasurement |
VIKINGZYSELJv20160909 |
error on Kron flux (SE: FLUXERR_AUTO; CASU: default) {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vikingMapRemeasurement |
VIKINGZYSELJv20170124 |
error on Kron flux (SE: FLUXERR_AUTO; CASU: default) {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCDR1 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCDR2 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCDR3 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCDR4 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCDR5 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20110909 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20120126 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20121128 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20130304 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20130805 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20140428 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20140903 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20150309 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20151218 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20160311 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20160822 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20170109 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20170411 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20171101 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20180702 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20181120 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20191212 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20210708 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20230816 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection |
VMCv20240226 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcDetection, vmcListRemeasurement |
VMCv20110816 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcdeepDetection |
VMCDEEPv20230713 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vmcdeepDetection |
VMCDEEPv20240506 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vvvDetection |
VVVDR1 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vvvDetection |
VVVDR2 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vvvDetection, vvvDetectionPawPrints, vvvDetectionTiles |
VVVDR5 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronFluxErr |
vvvDetection, vvvListRemeasurement |
VVVv20100531 |
error on Kron flux {catalogue TType keyword: Kron_flux_err} |
real |
4 |
ADU |
|
stat.error |
kronJky |
ultravistaMapRemeasurement |
ULTRAVISTADR4 |
Calibrated Kron flux within aperture r_k (CASU: default) |
real |
4 |
jansky |
|
phot.mag |
kronJky |
vikingMapRemeasurement |
VIKINGZYSELJv20160909 |
Calibrated Kron flux within aperture r_k (CASU: default) |
real |
4 |
jansky |
|
phot.mag |
kronJky |
vikingMapRemeasurement |
VIKINGZYSELJv20170124 |
Calibrated Kron flux within aperture r_k (CASU: default) |
real |
4 |
jansky |
|
phot.mag |
kronJkyErr |
ultravistaMapRemeasurement |
ULTRAVISTADR4 |
error on calibrated Kron flux |
real |
4 |
jansky (CASU: default) |
|
stat.error |
kronJkyErr |
vikingMapRemeasurement |
VIKINGZYSELJv20160909 |
error on calibrated Kron flux |
real |
4 |
jansky (CASU: default) |
|
stat.error |
kronJkyErr |
vikingMapRemeasurement |
VIKINGZYSELJv20170124 |
error on calibrated Kron flux |
real |
4 |
jansky (CASU: default) |
|
stat.error |
kronLup |
ultravistaMapRemeasurement |
ULTRAVISTADR4 |
Calibrated Kron luptitude within aperture r_k (CASU: default) |
real |
4 |
lup |
|
phot.mag |
kronLup |
vikingMapRemeasurement |
VIKINGZYSELJv20160909 |
Calibrated Kron luptitude within aperture r_k (CASU: default) |
real |
4 |
lup |
|
phot.mag |
kronLup |
vikingMapRemeasurement |
VIKINGZYSELJv20170124 |
Calibrated Kron luptitude within aperture r_k (CASU: default) |
real |
4 |
lup |
|
phot.mag |
kronLupErr |
ultravistaMapRemeasurement |
ULTRAVISTADR4 |
error on calibrated Kron luptitude |
real |
4 |
lup (CASU: default) |
|
stat.error |
kronLupErr |
vikingMapRemeasurement |
VIKINGZYSELJv20160909 |
error on calibrated Kron luptitude |
real |
4 |
lup (CASU: default) |
|
stat.error |
kronLupErr |
vikingMapRemeasurement |
VIKINGZYSELJv20170124 |
error on calibrated Kron luptitude |
real |
4 |
lup (CASU: default) |
|
stat.error |
kronMag |
sharksDetection |
SHARKSv20210222 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
sharksDetection |
SHARKSv20210421 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
ultravistaDetection |
ULTRAVISTADR4 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
ultravistaMapRemeasurement |
ULTRAVISTADR4 |
Calibrated Kron magnitude within aperture r_k (CASU: default) |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSDR2 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSDR3 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSDR4 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSDR5 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSDR6 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSv20120926 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSv20130417 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSv20140409 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSv20150108 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSv20160114 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSv20160507 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSv20170630 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSv20180419 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSv20201209 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSv20231101 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection |
VHSv20240731 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vhsDetection, vhsListRemeasurement |
VHSDR1 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
videoDetection |
VIDEODR2 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
videoDetection |
VIDEODR3 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
videoDetection |
VIDEODR4 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
videoDetection |
VIDEODR5 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
videoDetection |
VIDEOv20111208 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
videoDetection, videoListRemeasurement |
VIDEOv20100513 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingDetection |
VIKINGDR2 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingDetection |
VIKINGDR3 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingDetection |
VIKINGDR4 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingDetection |
VIKINGv20111019 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingDetection |
VIKINGv20130417 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingDetection |
VIKINGv20140402 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingDetection |
VIKINGv20150421 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingDetection |
VIKINGv20151230 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingDetection |
VIKINGv20160406 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingDetection |
VIKINGv20161202 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingDetection |
VIKINGv20170715 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingDetection, vikingListRemeasurement |
VIKINGv20110714 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingMapRemeasurement |
VIKINGZYSELJv20160909 |
Calibrated Kron magnitude within aperture r_k (CASU: default) |
real |
4 |
mag |
|
phot.mag |
kronMag |
vikingMapRemeasurement |
VIKINGZYSELJv20170124 |
Calibrated Kron magnitude within aperture r_k (CASU: default) |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCDR1 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCDR2 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCDR3 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCDR4 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCDR5 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20110909 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20120126 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20121128 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20130304 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20130805 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20140428 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20140903 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20150309 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20151218 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20160311 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20160822 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20170109 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20170411 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20171101 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20180702 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20181120 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20191212 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20210708 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20230816 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection |
VMCv20240226 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcDetection, vmcListRemeasurement |
VMCv20110816 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcdeepDetection |
VMCDEEPv20230713 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vmcdeepDetection |
VMCDEEPv20240506 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vvvDetection |
VVVDR1 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vvvDetection |
VVVDR2 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vvvDetection, vvvDetectionPawPrints, vvvDetectionTiles |
VVVDR5 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMag |
vvvDetection, vvvListRemeasurement |
VVVv20100531 |
Calibrated Kron magnitude within circular aperture r_k |
real |
4 |
mag |
|
phot.mag |
kronMagErr |
sharksDetection |
SHARKSv20210222 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
sharksDetection |
SHARKSv20210421 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
ultravistaDetection |
ULTRAVISTADR4 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
ultravistaMapRemeasurement |
ULTRAVISTADR4 |
error on calibrated Kron magnitude |
real |
4 |
mag (CASU: default) |
|
stat.error |
kronMagErr |
vhsDetection |
VHSDR2 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vhsDetection |
VHSDR3 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vhsDetection |
VHSDR4 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vhsDetection |
VHSDR5 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vhsDetection |
VHSDR6 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vhsDetection |
VHSv20120926 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vhsDetection |
VHSv20130417 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vhsDetection |
VHSv20140409 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vhsDetection |
VHSv20150108 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vhsDetection |
VHSv20160114 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vhsDetection |
VHSv20160507 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vhsDetection |
VHSv20170630 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vhsDetection |
VHSv20180419 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vhsDetection |
VHSv20201209 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vhsDetection |
VHSv20231101 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vhsDetection |
VHSv20240731 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vhsDetection, vhsListRemeasurement |
VHSDR1 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
videoDetection |
VIDEODR2 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
videoDetection |
VIDEODR3 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
videoDetection |
VIDEODR4 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
videoDetection |
VIDEODR5 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
videoDetection |
VIDEOv20111208 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
videoDetection, videoListRemeasurement |
VIDEOv20100513 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vikingDetection |
VIKINGDR2 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vikingDetection |
VIKINGDR3 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vikingDetection |
VIKINGDR4 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vikingDetection |
VIKINGv20111019 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vikingDetection |
VIKINGv20130417 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vikingDetection |
VIKINGv20140402 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vikingDetection |
VIKINGv20150421 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vikingDetection |
VIKINGv20151230 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vikingDetection |
VIKINGv20160406 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vikingDetection |
VIKINGv20161202 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vikingDetection |
VIKINGv20170715 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vikingDetection, vikingListRemeasurement |
VIKINGv20110714 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vikingMapRemeasurement |
VIKINGZYSELJv20160909 |
error on calibrated Kron magnitude |
real |
4 |
mag (CASU: default) |
|
stat.error |
kronMagErr |
vikingMapRemeasurement |
VIKINGZYSELJv20170124 |
error on calibrated Kron magnitude |
real |
4 |
mag (CASU: default) |
|
stat.error |
kronMagErr |
vmcDetection |
VMCDR1 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vmcDetection |
VMCDR2 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vmcDetection |
VMCDR3 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCDR4 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCDR5 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20110909 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vmcDetection |
VMCv20120126 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vmcDetection |
VMCv20121128 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vmcDetection |
VMCv20130304 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vmcDetection |
VMCv20130805 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vmcDetection |
VMCv20140428 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vmcDetection |
VMCv20140903 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20150309 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20151218 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20160311 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20160822 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20170109 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20170411 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20171101 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20180702 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20181120 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20191212 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20210708 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20230816 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection |
VMCv20240226 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcDetection, vmcListRemeasurement |
VMCv20110816 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vmcdeepDetection |
VMCDEEPv20230713 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vmcdeepDetection |
VMCDEEPv20240506 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vvvDetection |
VVVDR1 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vvvDetection |
VVVDR2 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronMagErr |
vvvDetection, vvvDetectionPawPrints, vvvDetectionTiles |
VVVDR5 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error;phot.mag |
kronMagErr |
vvvDetection, vvvListRemeasurement |
VVVv20100531 |
error on calibrated Kron magnitude |
real |
4 |
mag |
|
stat.error |
kronRad |
Detection |
PS1DR2 |
Kron (1980) radius. |
real |
4 |
arcsec |
-999 |
|
kronRad |
sharksDetection |
SHARKSv20210222 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
sharksDetection |
SHARKSv20210421 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
ultravistaDetection |
ULTRAVISTADR4 |
Kron radius as defined in SE by Graham and Driver (2005) (SE: KRON_RADIUS*A_IMAGE) {catalogue TType keyword: Kron_radius} r_k = ∑R² I(R) / ∑R I(R) |
real |
4 |
pixels |
|
phys.angSize |
Since <FLUX>_RADIUS is expressed in multiples of the major axis, <FLUX>_RADIUS is multiplied by A_IMAGE to convert to pixels. |
kronRad |
ultravistaMapRemeasurement |
ULTRAVISTADR4 |
Kron radius as defined in SE by Graham and Driver (2005) (SE: KRON_RADIUS*A_IMAGE; CASU: default) {catalogue TType keyword: Kron_radius} r_k = ∑R² I(R) / ∑R I(R) |
real |
4 |
pixels |
|
phys.angSize |
Since <FLUX>_RADIUS is expressed in multiples of the major axis, <FLUX>_RADIUS is multiplied by A_IMAGE to convert to pixels. |
kronRad |
vhsDetection |
VHSDR2 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize;src |
kronRad |
vhsDetection |
VHSDR3 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSDR4 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSDR5 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSDR6 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSv20120926 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSv20130417 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSv20140409 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSv20150108 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSv20160114 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSv20160507 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSv20170630 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSv20180419 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSv20201209 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSv20231101 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection |
VHSv20240731 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vhsDetection, vhsListRemeasurement |
VHSDR1 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize;src |
kronRad |
videoDetection |
VIDEODR2 |
Kron radius as defined in SE by Graham and Driver (2005) (SE: KRON_RADIUS*A_IMAGE) {catalogue TType keyword: Kron_radius} r_k = ∑R² I(R) / ∑R I(R) |
real |
4 |
pixels |
|
phys.angSize;src |
Since <FLUX>_RADIUS is expressed in multiples of the major axis, <FLUX>_RADIUS is multiplied by A_IMAGE to convert to pixels. |
kronRad |
videoDetection |
VIDEODR3 |
Kron radius as defined in SE by Graham and Driver (2005) (SE: KRON_RADIUS*A_IMAGE) {catalogue TType keyword: Kron_radius} r_k = ∑R² I(R) / ∑R I(R) |
real |
4 |
pixels |
|
phys.angSize |
Since <FLUX>_RADIUS is expressed in multiples of the major axis, <FLUX>_RADIUS is multiplied by A_IMAGE to convert to pixels. |
kronRad |
videoDetection |
VIDEODR4 |
Kron radius as defined in SE by Graham and Driver (2005) (SE: KRON_RADIUS*A_IMAGE) {catalogue TType keyword: Kron_radius} r_k = ∑R² I(R) / ∑R I(R) |
real |
4 |
pixels |
|
phys.angSize |
Since <FLUX>_RADIUS is expressed in multiples of the major axis, <FLUX>_RADIUS is multiplied by A_IMAGE to convert to pixels. |
kronRad |
videoDetection |
VIDEODR5 |
Kron radius as defined in SE by Graham and Driver (2005) (SE: KRON_RADIUS*A_IMAGE) {catalogue TType keyword: Kron_radius} r_k = ∑R² I(R) / ∑R I(R) |
real |
4 |
pixels |
|
phys.angSize |
Since <FLUX>_RADIUS is expressed in multiples of the major axis, <FLUX>_RADIUS is multiplied by A_IMAGE to convert to pixels. |
kronRad |
videoDetection |
VIDEOv20100513 |
Kron radius as defined in SE by Graham and Driver (2005) (SE: KRON_RADIUS*A_IMAGE) {catalogue TType keyword: Kron_radius} r_k = ∑R² I(R) / ∑R I(R) |
real |
4 |
pixels |
|
phys.angSize;src |
Since <FLUX>_RADIUS is expressed in multiples of the major axis, <FLUX>_RADIUS is multiplied by A_IMAGE to convert to pixels. |
kronRad |
videoDetection |
VIDEOv20111208 |
Kron radius as defined in SE by Graham and Driver (2005) (SE: KRON_RADIUS*A_IMAGE) {catalogue TType keyword: Kron_radius} r_k = ∑R² I(R) / ∑R I(R) |
real |
4 |
pixels |
|
phys.angSize;src |
Since <FLUX>_RADIUS is expressed in multiples of the major axis, <FLUX>_RADIUS is multiplied by A_IMAGE to convert to pixels. |
kronRad |
videoListRemeasurement |
VIDEOv20100513 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize;src |
kronRad |
vikingDetection |
VIKINGDR2 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize;src |
kronRad |
vikingDetection |
VIKINGDR3 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vikingDetection |
VIKINGDR4 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vikingDetection |
VIKINGv20111019 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize;src |
kronRad |
vikingDetection |
VIKINGv20130417 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vikingDetection |
VIKINGv20140402 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vikingDetection |
VIKINGv20150421 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vikingDetection |
VIKINGv20151230 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vikingDetection |
VIKINGv20160406 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vikingDetection |
VIKINGv20161202 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vikingDetection |
VIKINGv20170715 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vikingDetection, vikingListRemeasurement |
VIKINGv20110714 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize;src |
kronRad |
vikingMapRemeasurement |
VIKINGZYSELJv20160909 |
Kron radius as defined in SE by Graham and Driver (2005) (SE: KRON_RADIUS*A_IMAGE; CASU: default) {catalogue TType keyword: Kron_radius} r_k = ∑R² I(R) / ∑R I(R) |
real |
4 |
pixels |
|
phys.angSize;src |
Since <FLUX>_RADIUS is expressed in multiples of the major axis, <FLUX>_RADIUS is multiplied by A_IMAGE to convert to pixels. |
kronRad |
vikingMapRemeasurement |
VIKINGZYSELJv20170124 |
Kron radius as defined in SE by Graham and Driver (2005) (SE: KRON_RADIUS*A_IMAGE; CASU: default) {catalogue TType keyword: Kron_radius} r_k = ∑R² I(R) / ∑R I(R) |
real |
4 |
pixels |
|
phys.angSize;src |
Since <FLUX>_RADIUS is expressed in multiples of the major axis, <FLUX>_RADIUS is multiplied by A_IMAGE to convert to pixels. |
kronRad |
vmcDetection |
VMCDR1 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize;src |
kronRad |
vmcDetection |
VMCDR2 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCDR3 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCDR4 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCDR5 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20110909 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize;src |
kronRad |
vmcDetection |
VMCv20120126 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize;src |
kronRad |
vmcDetection |
VMCv20121128 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20130304 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20130805 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20140428 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20140903 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20150309 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20151218 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20160311 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20160822 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20170109 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20170411 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20171101 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20180702 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20181120 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20191212 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20210708 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20230816 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection |
VMCv20240226 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcDetection, vmcListRemeasurement |
VMCv20110816 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize;src |
kronRad |
vmcdeepDetection |
VMCDEEPv20230713 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vmcdeepDetection |
VMCDEEPv20240506 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vvvDetection |
VVVDR1 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vvvDetection |
VVVDR2 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vvvDetection, vvvDetectionPawPrints, vvvDetectionTiles |
VVVDR5 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize |
kronRad |
vvvDetection, vvvListRemeasurement |
VVVv20100531 |
r_k as defined in Bertin and Arnouts 1996 A&A Supp 117 393 {catalogue TType keyword: Kron_radius} |
real |
4 |
pixels |
|
phys.angSize;src |
ks_1AperMag1 |
vvvSource |
VVVDR5 |
Point source Ks_1 aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ks_1AperMag1Err |
vvvSource |
VVVDR5 |
Error in point source Ks_1 mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ks_1AperMag3 |
vvvSource |
VVVDR5 |
Default point source Ks_1 aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ks_1AperMag3Err |
vvvSource |
VVVDR5 |
Error in default point source Ks_1 mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ks_1AperMag4 |
vvvSource |
VVVDR5 |
Point source Ks_1 aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ks_1AperMag4Err |
vvvSource |
VVVDR5 |
Error in point source Ks_1 mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ks_1AverageConf |
vvvSource |
VVVDR5 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks_1 |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ks_1Class |
vvvSource |
VVVDR5 |
discrete image classification flag in Ks_1 |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ks_1ClassStat |
vvvSource |
VVVDR5 |
S-Extractor classification statistic in Ks_1 |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ks_1Ell |
vvvSource |
VVVDR5 |
1-b/a, where a/b=semi-major/minor axes in Ks_1 |
real |
4 |
|
-0.9999995e9 |
src.ellipticity;em.IR.K |
ks_1eNum |
vvvMergeLog |
VVVDR5 |
the extension number of this Ks_1 frame |
tinyint |
1 |
|
|
meta.number;em.IR.K |
ks_1eNum |
vvvPsfDophotZYJHKsMergeLog |
VVVDR5 |
the extension number of this 1st epoch Ks frame |
tinyint |
1 |
|
|
meta.number;em.IR.K |
ks_1ErrBits |
vvvSource |
VVVDR5 |
processing warning/error bitwise flags in Ks_1 |
int |
4 |
|
-99999999 |
meta.code;em.IR.K |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
ks_1Eta |
vvvSource |
VVVDR5 |
Offset of Ks_1 detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff;em.IR.K |
When associating individual passband detections into merged sources, a generous (in terms of the positional uncertainties) pairing radius of 1.0 arcseconds is used. Such a large association criterion can of course lead to spurious pairings in the merged sources lists (although note that between passband pairs, handshake pairing is done: both passbands must agree that the candidate pair is their nearest neighbour for the pair to propagate through into the merged source table). In order to help filter spurious pairings out, and assuming that large positional offsets between the different passband detections are not expected (e.g. because of source motion, or larger than usual positional uncertainties) then the attributes Xi and Eta can be used to filter any pairings with suspiciously large offsets in one or more bands. For example, for a clean sample of QSOs from the VHS, you might wish to insist that the offsets in the selected sample are all below 0.5 arcsecond: simply add WHERE clauses into the SQL sample selection script to exclude all Xi and Eta values larger than the threshold you want. NB: the master position is the position of the detection in the shortest passband in the set, rather than the ra/dec of the source as stored in source attributes of the same name. The former is used in the pairing process, while the latter is generally the optimally weighted mean position from an astrometric solution or other combinatorial process of all individual detection positions across the available passbands. |
ks_1Gausig |
vvvSource |
VVVDR5 |
RMS of axes of ellipse fit in Ks_1 |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param;em.IR.K |
ks_1mfID |
vvvMergeLog |
VVVDR5 |
the UID of the relevant Ks_1 multiframe |
bigint |
8 |
|
|
meta.id;obs.field;em.IR.K |
ks_1mfID |
vvvPsfDophotZYJHKsMergeLog |
VVVDR5 |
the UID of the relevant 1st epoch Ks tile multiframe |
bigint |
8 |
|
|
meta.id;obs.field;em.IR.K |
ks_1Mjd |
vvvPsfDophotZYJHKsMergeLog |
VVVDR5 |
the MJD of the 1st epoch Ks tile multiframe |
float |
8 |
|
|
time;em.IR.K |
ks_1Mjd |
vvvSource |
VVVDR5 |
Modified Julian Day in Ks_1 band |
float |
8 |
days |
-0.9999995e9 |
time.epoch;em.IR.K |
ks_1PA |
vvvSource |
VVVDR5 |
ellipse fit celestial orientation in Ks_1 |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng;em.IR.K |
ks_1ppErrBits |
vvvSource |
VVVDR5 |
additional WFAU post-processing error bits in Ks_1 |
int |
4 |
|
0 |
meta.code;em.IR.K |
ks_1SeqNum |
vvvSource |
VVVDR5 |
the running number of the Ks_1 detection |
int |
4 |
|
-99999999 |
meta.number;em.IR.K |
ks_1Xi |
vvvSource |
VVVDR5 |
Offset of Ks_1 detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff;em.IR.K |
When associating individual passband detections into merged sources, a generous (in terms of the positional uncertainties) pairing radius of 1.0 arcseconds is used. Such a large association criterion can of course lead to spurious pairings in the merged sources lists (although note that between passband pairs, handshake pairing is done: both passbands must agree that the candidate pair is their nearest neighbour for the pair to propagate through into the merged source table). In order to help filter spurious pairings out, and assuming that large positional offsets between the different passband detections are not expected (e.g. because of source motion, or larger than usual positional uncertainties) then the attributes Xi and Eta can be used to filter any pairings with suspiciously large offsets in one or more bands. For example, for a clean sample of QSOs from the VHS, you might wish to insist that the offsets in the selected sample are all below 0.5 arcsecond: simply add WHERE clauses into the SQL sample selection script to exclude all Xi and Eta values larger than the threshold you want. NB: the master position is the position of the detection in the shortest passband in the set, rather than the ra/dec of the source as stored in source attributes of the same name. The former is used in the pairing process, while the latter is generally the optimally weighted mean position from an astrometric solution or other combinatorial process of all individual detection positions across the available passbands. |
ks_2AperMag1 |
vvvSource |
VVVDR5 |
Point source Ks_2 aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ks_2AperMag1Err |
vvvSource |
VVVDR5 |
Error in point source Ks_2 mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ks_2AperMag3 |
vvvSource |
VVVDR5 |
Default point source Ks_2 aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ks_2AperMag3Err |
vvvSource |
VVVDR5 |
Error in default point source Ks_2 mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ks_2AperMag4 |
vvvSource |
VVVDR5 |
Point source Ks_2 aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ks_2AperMag4Err |
vvvSource |
VVVDR5 |
Error in point source Ks_2 mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ks_2AverageConf |
vvvSource |
VVVDR5 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks_2 |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ks_2Class |
vvvSource |
VVVDR5 |
discrete image classification flag in Ks_2 |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ks_2ClassStat |
vvvSource |
VVVDR5 |
S-Extractor classification statistic in Ks_2 |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ks_2Ell |
vvvSource |
VVVDR5 |
1-b/a, where a/b=semi-major/minor axes in Ks_2 |
real |
4 |
|
-0.9999995e9 |
src.ellipticity;em.IR.K |
ks_2eNum |
vvvMergeLog |
VVVDR5 |
the extension number of this Ks_2 frame |
tinyint |
1 |
|
|
meta.number;em.IR.K |
ks_2eNum |
vvvPsfDophotZYJHKsMergeLog |
VVVDR5 |
the extension number of this 2nd epoch Ks frame |
tinyint |
1 |
|
|
meta.number;em.IR.K |
ks_2ErrBits |
vvvSource |
VVVDR5 |
processing warning/error bitwise flags in Ks_2 |
int |
4 |
|
-99999999 |
meta.code;em.IR.K |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
ks_2Eta |
vvvSource |
VVVDR5 |
Offset of Ks_2 detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff;em.IR.K |
When associating individual passband detections into merged sources, a generous (in terms of the positional uncertainties) pairing radius of 1.0 arcseconds is used. Such a large association criterion can of course lead to spurious pairings in the merged sources lists (although note that between passband pairs, handshake pairing is done: both passbands must agree that the candidate pair is their nearest neighbour for the pair to propagate through into the merged source table). In order to help filter spurious pairings out, and assuming that large positional offsets between the different passband detections are not expected (e.g. because of source motion, or larger than usual positional uncertainties) then the attributes Xi and Eta can be used to filter any pairings with suspiciously large offsets in one or more bands. For example, for a clean sample of QSOs from the VHS, you might wish to insist that the offsets in the selected sample are all below 0.5 arcsecond: simply add WHERE clauses into the SQL sample selection script to exclude all Xi and Eta values larger than the threshold you want. NB: the master position is the position of the detection in the shortest passband in the set, rather than the ra/dec of the source as stored in source attributes of the same name. The former is used in the pairing process, while the latter is generally the optimally weighted mean position from an astrometric solution or other combinatorial process of all individual detection positions across the available passbands. |
ks_2Gausig |
vvvSource |
VVVDR5 |
RMS of axes of ellipse fit in Ks_2 |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param;em.IR.K |
ks_2mfID |
vvvMergeLog |
VVVDR5 |
the UID of the relevant Ks_2 multiframe |
bigint |
8 |
|
|
meta.id;obs.field;em.IR.K |
ks_2mfID |
vvvPsfDophotZYJHKsMergeLog |
VVVDR5 |
the UID of the relevant 2nd epoch Ks tile multiframe |
bigint |
8 |
|
|
meta.id;obs.field;em.IR.K |
ks_2Mjd |
vvvPsfDophotZYJHKsMergeLog |
VVVDR5 |
the MJD of the 2nd epoch Ks tile multiframe |
float |
8 |
|
|
time;em.IR.K |
ks_2Mjd |
vvvSource |
VVVDR5 |
Modified Julian Day in Ks_2 band |
float |
8 |
days |
-0.9999995e9 |
time.epoch;em.IR.K |
ks_2PA |
vvvSource |
VVVDR5 |
ellipse fit celestial orientation in Ks_2 |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng;em.IR.K |
ks_2ppErrBits |
vvvSource |
VVVDR5 |
additional WFAU post-processing error bits in Ks_2 |
int |
4 |
|
0 |
meta.code;em.IR.K |
ks_2SeqNum |
vvvSource |
VVVDR5 |
the running number of the Ks_2 detection |
int |
4 |
|
-99999999 |
meta.number;em.IR.K |
ks_2Xi |
vvvSource |
VVVDR5 |
Offset of Ks_2 detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff;em.IR.K |
When associating individual passband detections into merged sources, a generous (in terms of the positional uncertainties) pairing radius of 1.0 arcseconds is used. Such a large association criterion can of course lead to spurious pairings in the merged sources lists (although note that between passband pairs, handshake pairing is done: both passbands must agree that the candidate pair is their nearest neighbour for the pair to propagate through into the merged source table). In order to help filter spurious pairings out, and assuming that large positional offsets between the different passband detections are not expected (e.g. because of source motion, or larger than usual positional uncertainties) then the attributes Xi and Eta can be used to filter any pairings with suspiciously large offsets in one or more bands. For example, for a clean sample of QSOs from the VHS, you might wish to insist that the offsets in the selected sample are all below 0.5 arcsecond: simply add WHERE clauses into the SQL sample selection script to exclude all Xi and Eta values larger than the threshold you want. NB: the master position is the position of the detection in the shortest passband in the set, rather than the ra/dec of the source as stored in source attributes of the same name. The former is used in the pairing process, while the latter is generally the optimally weighted mean position from an astrometric solution or other combinatorial process of all individual detection positions across the available passbands. |
ksAmpl |
vmcCepheidVariables |
VMCDR3 |
Amplitude of Ks band magnitude variation {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCDR4 |
Peak-to-Peak amplitude in Ks band {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20121128 |
Amplitude of Ks band magnitude variation {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.NIR |
ksAmpl |
vmcCepheidVariables |
VMCv20140428 |
Amplitude of Ks band magnitude variation {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20140903 |
Amplitude of Ks band magnitude variation {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20150309 |
Amplitude of Ks band magnitude variation {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20151218 |
Amplitude of Ks band magnitude variation {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20160311 |
Peak-to-Peak amplitude in Ks band {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20160822 |
Peak-to-Peak amplitude in Ks band {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20170109 |
Peak-to-Peak amplitude in Ks band {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20170411 |
Peak-to-Peak amplitude in Ks band {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20171101 |
Peak-to-Peak amplitude in Ks band {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20180702 |
Peak-to-Peak amplitude in Ks band {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20181120 |
Peak-to-Peak amplitude in Ks band {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20191212 |
Peak-to-Peak amplitude in Ks band {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20210708 |
Peak-to-Peak amplitude in Ks band {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20230816 |
Peak-to-Peak amplitude in Ks band {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcCepheidVariables |
VMCv20240226 |
Peak-to-Peak amplitude in Ks band {catalogue TType keyword: A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcRRlyraeVariables |
VMCDR4 |
Amplitude in K_s band provided by GRATIS {catalogue TType keyword: AMPL_K} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcRRlyraeVariables |
VMCv20160822 |
Amplitude in K_s band provided by GRATIS {catalogue TType keyword: AMPL_K} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcRRlyraeVariables |
VMCv20170109 |
Amplitude in K_s band provided by GRATIS {catalogue TType keyword: AMPL_K} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcRRlyraeVariables |
VMCv20170411 |
Amplitude in K_s band provided by GRATIS {catalogue TType keyword: AMPL_K} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcRRlyraeVariables |
VMCv20171101 |
Amplitude in K_s band provided by GRATIS {catalogue TType keyword: AMPL_K} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcRRlyraeVariables |
VMCv20180702 |
Amplitude in K_s band provided by GRATIS {catalogue TType keyword: AMPL_K} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcRRlyraeVariables |
VMCv20181120 |
Amplitude in K_s band provided by GRATIS {catalogue TType keyword: AMPL_K} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcRRlyraeVariables |
VMCv20191212 |
Amplitude in K_s band provided by GRATIS {catalogue TType keyword: AMPL_K} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcRRlyraeVariables |
VMCv20210708 |
Amplitude in K_s band provided by GRATIS {catalogue TType keyword: AMPL_K} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmpl |
vmcRRlyraeVariables |
VMCv20230816 |
Amplitude in K_s band provided by GRATIS {catalogue TType keyword: AMPL_K} |
real |
4 |
mag |
-0.9999995e9 |
src.var.amplitude;em.IR.K |
ksAmplErr |
vmcCepheidVariables |
VMCDR4 |
Error in Peak-to-Peak amplitude in Ks band {catalogue TType keyword: e_A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
stat.error;src.var.amplitude;em.IR.K |
ksAmplErr |
vmcCepheidVariables |
VMCv20160311 |
Error in Peak-to-Peak amplitude in Ks band {catalogue TType keyword: e_A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
stat.error;src.var.amplitude;em.IR.K |
ksAmplErr |
vmcCepheidVariables |
VMCv20160822 |
Error in Peak-to-Peak amplitude in Ks band {catalogue TType keyword: e_A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
stat.error;src.var.amplitude;em.IR.K |
ksAmplErr |
vmcCepheidVariables |
VMCv20170109 |
Error in Peak-to-Peak amplitude in Ks band {catalogue TType keyword: e_A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
stat.error;src.var.amplitude;em.IR.K |
ksAmplErr |
vmcCepheidVariables |
VMCv20170411 |
Error in Peak-to-Peak amplitude in Ks band {catalogue TType keyword: e_A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
stat.error;src.var.amplitude;em.IR.K |
ksAmplErr |
vmcCepheidVariables |
VMCv20171101 |
Error in Peak-to-Peak amplitude in Ks band {catalogue TType keyword: e_A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
stat.error;src.var.amplitude;em.IR.K |
ksAmplErr |
vmcCepheidVariables |
VMCv20180702 |
Error in Peak-to-Peak amplitude in Ks band {catalogue TType keyword: e_A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
stat.error;src.var.amplitude;em.IR.K |
ksAmplErr |
vmcCepheidVariables |
VMCv20181120 |
Error in Peak-to-Peak amplitude in Ks band {catalogue TType keyword: e_A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
stat.error;src.var.amplitude;em.IR.K |
ksAmplErr |
vmcCepheidVariables |
VMCv20191212 |
Error in Peak-to-Peak amplitude in Ks band {catalogue TType keyword: e_A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
stat.error;src.var.amplitude;em.IR.K |
ksAmplErr |
vmcCepheidVariables |
VMCv20210708 |
Error in Peak-to-Peak amplitude in Ks band {catalogue TType keyword: e_A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
stat.error;src.var.amplitude;em.IR.K |
ksAmplErr |
vmcCepheidVariables |
VMCv20230816 |
Error in Peak-to-Peak amplitude in Ks band {catalogue TType keyword: e_A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
stat.error;src.var.amplitude;em.IR.K |
ksAmplErr |
vmcCepheidVariables |
VMCv20240226 |
Error in Peak-to-Peak amplitude in Ks band {catalogue TType keyword: e_A(Ks)} |
real |
4 |
mag |
-0.9999995e9 |
stat.error;src.var.amplitude;em.IR.K |
ksAperJky3 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Default point source Ks aperture corrected (2.0 arcsec aperture diameter) calibrated flux If in doubt use this flux estimator |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJky3 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Default point source Ks aperture corrected (2.0 arcsec aperture diameter) calibrated flux If in doubt use this flux estimator |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJky3 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Default point source Ks aperture corrected (2.0 arcsec aperture diameter) calibrated flux If in doubt use this flux estimator |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJky3Err |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Error in default point/extended source Ks (2.0 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
stat.error |
ksAperJky3Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Error in default point/extended source Ks (2.0 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
stat.error |
ksAperJky3Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Error in default point/extended source Ks (2.0 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
stat.error |
ksAperJky4 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Point source Ks aperture corrected (2.8 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJky4 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Point source Ks aperture corrected (2.8 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJky4 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Point source Ks aperture corrected (2.8 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJky4Err |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Error in point/extended source Ks (2.8 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
stat.error |
ksAperJky4Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Error in point/extended source Ks (2.8 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
stat.error |
ksAperJky4Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Error in point/extended source Ks (2.8 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
stat.error |
ksAperJky6 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Point source Ks aperture corrected (5.7 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJky6 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Point source Ks aperture corrected (5.7 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJky6 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Point source Ks aperture corrected (5.7 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJky6Err |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Error in point/extended source Ks (5.7 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
stat.error |
ksAperJky6Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Error in point/extended source Ks (5.7 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
stat.error |
ksAperJky6Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Error in point/extended source Ks (5.7 arcsec aperture diameter) calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
stat.error |
ksAperJkyNoAperCorr3 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Default extended source Ks (2.0 arcsec aperture diameter, but no aperture correction applied) aperture calibrated flux If in doubt use this flux estimator |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJkyNoAperCorr3 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Default extended source Ks (2.0 arcsec aperture diameter, but no aperture correction applied) aperture calibrated flux If in doubt use this flux estimator |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJkyNoAperCorr3 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Default extended source Ks (2.0 arcsec aperture diameter, but no aperture correction applied) aperture calibrated flux If in doubt use this flux estimator |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJkyNoAperCorr4 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Extended source Ks (2.8 arcsec aperture diameter, but no aperture correction applied) aperture calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJkyNoAperCorr4 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Extended source Ks (2.8 arcsec aperture diameter, but no aperture correction applied) aperture calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJkyNoAperCorr4 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Extended source Ks (2.8 arcsec aperture diameter, but no aperture correction applied) aperture calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJkyNoAperCorr6 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Extended source Ks (5.7 arcsec aperture diameter, but no aperture correction applied) aperture calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJkyNoAperCorr6 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Extended source Ks (5.7 arcsec aperture diameter, but no aperture correction applied) aperture calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperJkyNoAperCorr6 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Extended source Ks (5.7 arcsec aperture diameter, but no aperture correction applied) aperture calibrated flux |
real |
4 |
jansky |
-0.9999995e9 |
phot.flux |
ksAperLup3 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Default point source Ks aperture corrected (2.0 arcsec aperture diameter) luptitude If in doubt use this flux estimator |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLup3 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Default point source Ks aperture corrected (2.0 arcsec aperture diameter) luptitude If in doubt use this flux estimator |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLup3 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Default point source Ks aperture corrected (2.0 arcsec aperture diameter) luptitude If in doubt use this flux estimator |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLup3Err |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Error in default point/extended source Ks (2.0 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
stat.error |
ksAperLup3Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Error in default point/extended source Ks (2.0 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
stat.error |
ksAperLup3Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Error in default point/extended source Ks (2.0 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
stat.error |
ksAperLup4 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Point source Ks aperture corrected (2.8 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLup4 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Point source Ks aperture corrected (2.8 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLup4 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Point source Ks aperture corrected (2.8 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLup4Err |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Error in point/extended source Ks (2.8 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
stat.error |
ksAperLup4Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Error in point/extended source Ks (2.8 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
stat.error |
ksAperLup4Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Error in point/extended source Ks (2.8 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
stat.error |
ksAperLup6 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Point source Ks aperture corrected (5.7 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLup6 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Point source Ks aperture corrected (5.7 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLup6 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Point source Ks aperture corrected (5.7 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLup6Err |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Error in point/extended source Ks (5.7 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
stat.error |
ksAperLup6Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Error in point/extended source Ks (5.7 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
stat.error |
ksAperLup6Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Error in point/extended source Ks (5.7 arcsec aperture diameter) luptitude |
real |
4 |
lup |
-0.9999995e9 |
stat.error |
ksAperLupNoAperCorr3 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Default extended source Ks (2.0 arcsec aperture diameter, but no aperture correction applied) aperture luptitude If in doubt use this flux estimator |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLupNoAperCorr3 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Default extended source Ks (2.0 arcsec aperture diameter, but no aperture correction applied) aperture luptitude If in doubt use this flux estimator |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLupNoAperCorr3 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Default extended source Ks (2.0 arcsec aperture diameter, but no aperture correction applied) aperture luptitude If in doubt use this flux estimator |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLupNoAperCorr4 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Extended source Ks (2.8 arcsec aperture diameter, but no aperture correction applied) aperture luptitude |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLupNoAperCorr4 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Extended source Ks (2.8 arcsec aperture diameter, but no aperture correction applied) aperture luptitude |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLupNoAperCorr4 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Extended source Ks (2.8 arcsec aperture diameter, but no aperture correction applied) aperture luptitude |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLupNoAperCorr6 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Extended source Ks (5.7 arcsec aperture diameter, but no aperture correction applied) aperture luptitude |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLupNoAperCorr6 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Extended source Ks (5.7 arcsec aperture diameter, but no aperture correction applied) aperture luptitude |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperLupNoAperCorr6 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Extended source Ks (5.7 arcsec aperture diameter, but no aperture correction applied) aperture luptitude |
real |
4 |
lup |
-0.9999995e9 |
phot.lup |
ksAperMag1 |
vmcSynopticSource |
VMCDR1 |
Extended source Ks aperture corrected mag (0.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag1 |
vmcSynopticSource |
VMCDR2 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCDR3 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCDR4 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCDR5 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20110816 |
Extended source Ks aperture corrected mag (0.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag1 |
vmcSynopticSource |
VMCv20110909 |
Extended source Ks aperture corrected mag (0.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag1 |
vmcSynopticSource |
VMCv20120126 |
Extended source Ks aperture corrected mag (0.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag1 |
vmcSynopticSource |
VMCv20121128 |
Extended source Ks aperture corrected mag (0.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag1 |
vmcSynopticSource |
VMCv20130304 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag1 |
vmcSynopticSource |
VMCv20130805 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20140428 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20140903 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20150309 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20151218 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20160311 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20160822 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20170109 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20170411 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20171101 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20180702 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20181120 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20191212 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20210708 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20230816 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcSynopticSource |
VMCv20240226 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcdeepSynopticSource |
VMCDEEPv20230713 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vmcdeepSynopticSource |
VMCDEEPv20240506 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vvvSource |
VVVDR1 |
Extended source Ks aperture corrected mag (0.7 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag1 |
vvvSource |
VVVDR5 |
Point source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1 |
vvvSource |
VVVv20100531 |
Extended source Ks aperture corrected mag (0.7 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag1 |
vvvSource |
VVVv20110718 |
Extended source Ks aperture corrected mag (0.7 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag1 |
vvvSource, vvvSynopticSource |
VVVDR2 |
Extended source Ks aperture corrected mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCDR1 |
Error in extended source Ks mag (0.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag1Err |
vmcSynopticSource |
VMCDR2 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag1Err |
vmcSynopticSource |
VMCDR3 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag1Err |
vmcSynopticSource |
VMCDR4 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCDR5 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20110816 |
Error in extended source Ks mag (0.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag1Err |
vmcSynopticSource |
VMCv20110909 |
Error in extended source Ks mag (0.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag1Err |
vmcSynopticSource |
VMCv20120126 |
Error in extended source Ks mag (0.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag1Err |
vmcSynopticSource |
VMCv20121128 |
Error in extended source Ks mag (0.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag1Err |
vmcSynopticSource |
VMCv20130304 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag1Err |
vmcSynopticSource |
VMCv20130805 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag1Err |
vmcSynopticSource |
VMCv20140428 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20140903 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag1Err |
vmcSynopticSource |
VMCv20150309 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag1Err |
vmcSynopticSource |
VMCv20151218 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20160311 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20160822 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20170109 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20170411 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20171101 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20180702 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20181120 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20191212 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20210708 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20230816 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcSynopticSource |
VMCv20240226 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcdeepSynopticSource |
VMCDEEPv20230713 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vmcdeepSynopticSource |
VMCDEEPv20240506 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vvvSource |
VVVDR1 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag1Err |
vvvSource |
VVVDR5 |
Error in point source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag1Err |
vvvSource |
VVVv20100531 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag1Err |
vvvSource |
VVVv20110718 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag1Err |
vvvSource, vvvSynopticSource |
VVVDR2 |
Error in extended source Ks mag (1.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag2 |
vmcSynopticSource |
VMCDR1 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag2 |
vmcSynopticSource |
VMCDR2 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCDR3 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCDR4 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCDR5 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20110816 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag2 |
vmcSynopticSource |
VMCv20110909 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag2 |
vmcSynopticSource |
VMCv20120126 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag2 |
vmcSynopticSource |
VMCv20121128 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag2 |
vmcSynopticSource |
VMCv20130304 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag2 |
vmcSynopticSource |
VMCv20130805 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20140428 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20140903 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20150309 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20151218 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20160311 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20160822 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20170109 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20170411 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20171101 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20180702 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20181120 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20191212 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20210708 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20230816 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcSynopticSource |
VMCv20240226 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcdeepSynopticSource |
VMCDEEPv20230713 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vmcdeepSynopticSource |
VMCDEEPv20240506 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2 |
vvvSynopticSource |
VVVDR1 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag2 |
vvvSynopticSource |
VVVDR2 |
Extended source Ks aperture corrected mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCDR1 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag2Err |
vmcSynopticSource |
VMCDR2 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag2Err |
vmcSynopticSource |
VMCDR3 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag2Err |
vmcSynopticSource |
VMCDR4 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCDR5 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20110816 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag2Err |
vmcSynopticSource |
VMCv20110909 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag2Err |
vmcSynopticSource |
VMCv20120126 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag2Err |
vmcSynopticSource |
VMCv20121128 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag2Err |
vmcSynopticSource |
VMCv20130304 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag2Err |
vmcSynopticSource |
VMCv20130805 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag2Err |
vmcSynopticSource |
VMCv20140428 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20140903 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag2Err |
vmcSynopticSource |
VMCv20150309 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag2Err |
vmcSynopticSource |
VMCv20151218 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20160311 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20160822 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20170109 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20170411 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20171101 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20180702 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20181120 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20191212 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20210708 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20230816 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcSynopticSource |
VMCv20240226 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcdeepSynopticSource |
VMCDEEPv20230713 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vmcdeepSynopticSource |
VMCDEEPv20240506 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag2Err |
vvvSynopticSource |
VVVDR1 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag2Err |
vvvSynopticSource |
VVVDR2 |
Error in extended source Ks mag (1.4 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3 |
sharksSource |
SHARKSv20210222 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
sharksSource |
SHARKSv20210421 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
ultravistaSource |
ULTRAVISTADR4 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Default point source Ks aperture corrected (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vhsSource |
VHSDR1 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vhsSource |
VHSDR2 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vhsSource |
VHSDR3 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vhsSource |
VHSDR4 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vhsSource |
VHSDR5 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vhsSource |
VHSDR6 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vhsSource |
VHSv20120926 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vhsSource |
VHSv20130417 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vhsSource |
VHSv20140409 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vhsSource |
VHSv20150108 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vhsSource |
VHSv20160114 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vhsSource |
VHSv20160507 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vhsSource |
VHSv20170630 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vhsSource |
VHSv20180419 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vhsSource |
VHSv20201209 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vhsSource |
VHSv20231101 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vhsSource |
VHSv20240731 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
videoSource |
VIDEODR2 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
videoSource |
VIDEODR3 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
videoSource |
VIDEODR4 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
videoSource |
VIDEODR5 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
videoSource |
VIDEOv20100513 |
Default point/extended source Ks mag, no aperture correction applied If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
videoSource |
VIDEOv20111208 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vikingSource |
VIKINGDR2 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vikingSource |
VIKINGDR3 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vikingSource |
VIKINGDR4 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vikingSource |
VIKINGv20110714 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vikingSource |
VIKINGv20111019 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vikingSource |
VIKINGv20130417 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vikingSource |
VIKINGv20140402 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vikingSource |
VIKINGv20150421 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vikingSource |
VIKINGv20151230 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vikingSource |
VIKINGv20160406 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vikingSource |
VIKINGv20161202 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vikingSource |
VIKINGv20170715 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Default point source Ks aperture corrected (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Default point source Ks aperture corrected (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSource |
VMCDR1 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSource |
VMCDR2 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCDR3 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCDR4 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCDR5 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20110816 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSource |
VMCv20110909 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSource |
VMCv20120126 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSource |
VMCv20121128 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSource |
VMCv20130304 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSource |
VMCv20130805 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20140428 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20140903 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20150309 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20151218 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20160311 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20160822 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20170109 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20170411 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20171101 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20180702 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20181120 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20191212 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20210708 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20230816 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSource |
VMCv20240226 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCDR1 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSynopticSource |
VMCDR2 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCDR3 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCDR4 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCDR5 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20110816 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSynopticSource |
VMCv20110909 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSynopticSource |
VMCv20120126 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSynopticSource |
VMCv20121128 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSynopticSource |
VMCv20130304 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vmcSynopticSource |
VMCv20130805 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20140428 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20140903 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20150309 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20151218 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20160311 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20160822 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20170109 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20170411 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20171101 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20180702 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20181120 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20191212 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20210708 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20230816 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcSynopticSource |
VMCv20240226 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcdeepSource |
VMCDEEPv20230713 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcdeepSource |
VMCDEEPv20240506 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcdeepSynopticSource |
VMCDEEPv20230713 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vmcdeepSynopticSource |
VMCDEEPv20240506 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vvvSource |
VVVDR1 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vvvSource |
VVVDR2 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vvvSource |
VVVDR5 |
Default point source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vvvSource |
VVVv20100531 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vvvSource |
VVVv20110718 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vvvSynopticSource |
VVVDR1 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag3 |
vvvSynopticSource |
VVVDR2 |
Default point/extended source Ks aperture corrected mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag3 |
vvvVivaCatalogue |
VVVDR5 |
ks magnitude using aperture corrected mag (2.0 arcsec aperture diameter, from VVVDR4 1st epoch JHKs contemporaneous OB) {catalogue TType keyword: ksAperMag3} |
real |
4 |
mag |
-9.999995e8 |
|
ksAperMag3Err |
sharksSource |
SHARKSv20210222 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
sharksSource |
SHARKSv20210421 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
ultravistaSource |
ULTRAVISTADR4 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Error in default point/extended source Ks (2.0 arcsec aperture diameter) magnitude |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vhsSource |
VHSDR1 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vhsSource |
VHSDR2 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vhsSource |
VHSDR3 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag3Err |
vhsSource |
VHSDR4 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag3Err |
vhsSource |
VHSDR5 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vhsSource |
VHSDR6 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vhsSource |
VHSv20120926 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vhsSource |
VHSv20130417 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vhsSource |
VHSv20140409 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag3Err |
vhsSource |
VHSv20150108 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag3Err |
vhsSource |
VHSv20160114 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vhsSource |
VHSv20160507 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vhsSource |
VHSv20170630 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vhsSource |
VHSv20180419 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vhsSource |
VHSv20201209 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vhsSource |
VHSv20231101 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vhsSource |
VHSv20240731 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
videoSource |
VIDEODR2 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
videoSource |
VIDEODR3 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
videoSource |
VIDEODR4 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag3Err |
videoSource |
VIDEODR5 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag3Err |
videoSource |
VIDEOv20100513 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
videoSource |
VIDEOv20111208 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vikingSource |
VIKINGDR2 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vikingSource |
VIKINGDR3 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vikingSource |
VIKINGDR4 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag3Err |
vikingSource |
VIKINGv20110714 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vikingSource |
VIKINGv20111019 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vikingSource |
VIKINGv20130417 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vikingSource |
VIKINGv20140402 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vikingSource |
VIKINGv20150421 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag3Err |
vikingSource |
VIKINGv20151230 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vikingSource |
VIKINGv20160406 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vikingSource |
VIKINGv20161202 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vikingSource |
VIKINGv20170715 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Error in default point/extended source Ks (2.0 arcsec aperture diameter) magnitude |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Error in default point/extended source Ks (2.0 arcsec aperture diameter) magnitude |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vmcSource |
VMCDR2 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vmcSource |
VMCDR3 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag3Err |
vmcSource |
VMCDR4 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCDR5 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20110816 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vmcSource |
VMCv20110909 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vmcSource |
VMCv20120126 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vmcSource |
VMCv20121128 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vmcSource |
VMCv20130304 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vmcSource |
VMCv20130805 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vmcSource |
VMCv20140428 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20140903 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag3Err |
vmcSource |
VMCv20150309 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag3Err |
vmcSource |
VMCv20151218 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20160311 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20160822 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20170109 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20170411 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20171101 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20180702 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20181120 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20191212 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20210708 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20230816 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource |
VMCv20240226 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcSource, vmcSynopticSource |
VMCDR1 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vmcdeepSource |
VMCDEEPv20240506 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vmcdeepSource, vmcdeepSynopticSource |
VMCDEEPv20230713 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vvvSource |
VVVDR2 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vvvSource |
VVVDR5 |
Error in default point source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag3Err |
vvvSource |
VVVv20100531 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vvvSource |
VVVv20110718 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vvvSource, vvvSynopticSource |
VVVDR1 |
Error in default point/extended source Ks mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag3Err |
vvvVivaCatalogue |
VVVDR5 |
Error in default point source Ks mag, from VVVDR4 {catalogue TType keyword: ksAperMag3Err} |
real |
4 |
mag |
-9.999995e8 |
|
ksAperMag4 |
sharksSource |
SHARKSv20210222 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
sharksSource |
SHARKSv20210421 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
ultravistaSource |
ULTRAVISTADR4 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Point source Ks aperture corrected (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vhsSource |
VHSDR1 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vhsSource |
VHSDR2 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vhsSource |
VHSDR3 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vhsSource |
VHSDR4 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vhsSource |
VHSDR5 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vhsSource |
VHSDR6 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vhsSource |
VHSv20120926 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vhsSource |
VHSv20130417 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vhsSource |
VHSv20140409 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vhsSource |
VHSv20150108 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vhsSource |
VHSv20160114 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vhsSource |
VHSv20160507 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vhsSource |
VHSv20170630 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vhsSource |
VHSv20180419 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vhsSource |
VHSv20201209 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vhsSource |
VHSv20231101 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vhsSource |
VHSv20240731 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
videoSource |
VIDEODR2 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
videoSource |
VIDEODR3 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
videoSource |
VIDEODR4 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
videoSource |
VIDEODR5 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
videoSource |
VIDEOv20100513 |
Extended source Ks mag, no aperture correction applied |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
videoSource |
VIDEOv20111208 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vikingSource |
VIKINGDR2 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vikingSource |
VIKINGDR3 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vikingSource |
VIKINGDR4 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vikingSource |
VIKINGv20110714 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vikingSource |
VIKINGv20111019 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vikingSource |
VIKINGv20130417 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vikingSource |
VIKINGv20140402 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vikingSource |
VIKINGv20150421 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vikingSource |
VIKINGv20151230 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vikingSource |
VIKINGv20160406 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vikingSource |
VIKINGv20161202 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vikingSource |
VIKINGv20170715 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Point source Ks aperture corrected (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Point source Ks aperture corrected (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSource |
VMCDR1 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSource |
VMCDR2 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCDR3 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCDR4 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCDR5 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20110816 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSource |
VMCv20110909 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSource |
VMCv20120126 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSource |
VMCv20121128 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSource |
VMCv20130304 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSource |
VMCv20130805 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20140428 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20140903 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20150309 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20151218 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20160311 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20160822 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20170109 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20170411 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20171101 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20180702 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20181120 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20191212 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20210708 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20230816 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSource |
VMCv20240226 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCDR1 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSynopticSource |
VMCDR2 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCDR3 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCDR4 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCDR5 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20110816 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSynopticSource |
VMCv20110909 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSynopticSource |
VMCv20120126 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSynopticSource |
VMCv20121128 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSynopticSource |
VMCv20130304 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vmcSynopticSource |
VMCv20130805 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20140428 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20140903 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20150309 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20151218 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20160311 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20160822 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20170109 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20170411 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20171101 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20180702 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20181120 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20191212 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20210708 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20230816 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcSynopticSource |
VMCv20240226 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcdeepSource |
VMCDEEPv20230713 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcdeepSource |
VMCDEEPv20240506 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcdeepSynopticSource |
VMCDEEPv20230713 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vmcdeepSynopticSource |
VMCDEEPv20240506 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vvvSource |
VVVDR2 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vvvSource |
VVVDR5 |
Point source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag4 |
vvvSource |
VVVv20100531 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vvvSource |
VVVv20110718 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4 |
vvvSource, vvvSynopticSource |
VVVDR1 |
Extended source Ks aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag4Err |
sharksSource |
SHARKSv20210222 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
sharksSource |
SHARKSv20210421 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
ultravistaSource |
ULTRAVISTADR4 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Error in point/extended source Ks (2.8 arcsec aperture diameter) magnitude |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vhsSource |
VHSDR1 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vhsSource |
VHSDR2 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vhsSource |
VHSDR3 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag4Err |
vhsSource |
VHSDR4 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag4Err |
vhsSource |
VHSDR5 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vhsSource |
VHSDR6 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vhsSource |
VHSv20120926 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vhsSource |
VHSv20130417 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vhsSource |
VHSv20140409 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag4Err |
vhsSource |
VHSv20150108 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag4Err |
vhsSource |
VHSv20160114 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vhsSource |
VHSv20160507 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vhsSource |
VHSv20170630 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vhsSource |
VHSv20180419 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vhsSource |
VHSv20201209 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vhsSource |
VHSv20231101 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vhsSource |
VHSv20240731 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
videoSource |
VIDEODR2 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
videoSource |
VIDEODR3 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
videoSource |
VIDEODR4 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag4Err |
videoSource |
VIDEODR5 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag4Err |
videoSource |
VIDEOv20100513 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
videoSource |
VIDEOv20111208 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vikingSource |
VIKINGDR2 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vikingSource |
VIKINGDR3 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vikingSource |
VIKINGDR4 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag4Err |
vikingSource |
VIKINGv20110714 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vikingSource |
VIKINGv20111019 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vikingSource |
VIKINGv20130417 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vikingSource |
VIKINGv20140402 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vikingSource |
VIKINGv20150421 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag4Err |
vikingSource |
VIKINGv20151230 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vikingSource |
VIKINGv20160406 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vikingSource |
VIKINGv20161202 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vikingSource |
VIKINGv20170715 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Error in point/extended source Ks (2.8 arcsec aperture diameter) magnitude |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Error in point/extended source Ks (2.8 arcsec aperture diameter) magnitude |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSource |
VMCDR1 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSource |
VMCDR2 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSource |
VMCDR3 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag4Err |
vmcSource |
VMCDR4 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCDR5 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20110816 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSource |
VMCv20110909 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSource |
VMCv20120126 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSource |
VMCv20121128 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSource |
VMCv20130304 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSource |
VMCv20130805 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSource |
VMCv20140428 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20140903 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag4Err |
vmcSource |
VMCv20150309 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag4Err |
vmcSource |
VMCv20151218 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20160311 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20160822 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20170109 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20170411 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20171101 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20180702 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20181120 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20191212 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20210708 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20230816 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSource |
VMCv20240226 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCDR1 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSynopticSource |
VMCDR2 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSynopticSource |
VMCDR3 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag4Err |
vmcSynopticSource |
VMCDR4 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCDR5 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20110816 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSynopticSource |
VMCv20110909 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSynopticSource |
VMCv20120126 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSynopticSource |
VMCv20121128 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSynopticSource |
VMCv20130304 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSynopticSource |
VMCv20130805 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vmcSynopticSource |
VMCv20140428 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20140903 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag4Err |
vmcSynopticSource |
VMCv20150309 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag4Err |
vmcSynopticSource |
VMCv20151218 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20160311 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20160822 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20170109 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20170411 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20171101 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20180702 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20181120 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20191212 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20210708 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20230816 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcSynopticSource |
VMCv20240226 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcdeepSource |
VMCDEEPv20230713 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcdeepSource |
VMCDEEPv20240506 |
Error in point/extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcdeepSynopticSource |
VMCDEEPv20230713 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vmcdeepSynopticSource |
VMCDEEPv20240506 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vvvSource |
VVVDR2 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vvvSource |
VVVDR5 |
Error in point source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag4Err |
vvvSource |
VVVv20100531 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vvvSource |
VVVv20110718 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag4Err |
vvvSource, vvvSynopticSource |
VVVDR1 |
Error in extended source Ks mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag5 |
vmcSynopticSource |
VMCDR1 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag5 |
vmcSynopticSource |
VMCDR2 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCDR3 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCDR4 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCDR5 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20110816 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag5 |
vmcSynopticSource |
VMCv20110909 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag5 |
vmcSynopticSource |
VMCv20120126 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag5 |
vmcSynopticSource |
VMCv20121128 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag5 |
vmcSynopticSource |
VMCv20130304 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag5 |
vmcSynopticSource |
VMCv20130805 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20140428 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20140903 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20150309 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20151218 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20160311 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20160822 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20170109 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20170411 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20171101 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20180702 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20181120 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20191212 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20210708 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20230816 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcSynopticSource |
VMCv20240226 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcdeepSynopticSource |
VMCDEEPv20230713 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vmcdeepSynopticSource |
VMCDEEPv20240506 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5 |
vvvSynopticSource |
VVVDR1 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag5 |
vvvSynopticSource |
VVVDR2 |
Extended source Ks aperture corrected mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCDR1 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag5Err |
vmcSynopticSource |
VMCDR2 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag5Err |
vmcSynopticSource |
VMCDR3 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag5Err |
vmcSynopticSource |
VMCDR4 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCDR5 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20110816 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag5Err |
vmcSynopticSource |
VMCv20110909 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag5Err |
vmcSynopticSource |
VMCv20120126 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag5Err |
vmcSynopticSource |
VMCv20121128 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag5Err |
vmcSynopticSource |
VMCv20130304 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag5Err |
vmcSynopticSource |
VMCv20130805 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag5Err |
vmcSynopticSource |
VMCv20140428 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20140903 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag5Err |
vmcSynopticSource |
VMCv20150309 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag5Err |
vmcSynopticSource |
VMCv20151218 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20160311 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20160822 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20170109 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20170411 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20171101 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20180702 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20181120 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20191212 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20210708 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20230816 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcSynopticSource |
VMCv20240226 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcdeepSynopticSource |
VMCDEEPv20230713 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vmcdeepSynopticSource |
VMCDEEPv20240506 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag5Err |
vvvSynopticSource |
VVVDR1 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag5Err |
vvvSynopticSource |
VVVDR2 |
Error in extended source Ks mag (4.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6 |
sharksSource |
SHARKSv20210222 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
sharksSource |
SHARKSv20210421 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
ultravistaSource |
ULTRAVISTADR4 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Point source Ks aperture corrected (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vhsSource |
VHSDR1 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vhsSource |
VHSDR2 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vhsSource |
VHSDR3 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vhsSource |
VHSDR4 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vhsSource |
VHSDR5 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vhsSource |
VHSDR6 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vhsSource |
VHSv20120926 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vhsSource |
VHSv20130417 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vhsSource |
VHSv20140409 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vhsSource |
VHSv20150108 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vhsSource |
VHSv20160114 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vhsSource |
VHSv20160507 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vhsSource |
VHSv20170630 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vhsSource |
VHSv20180419 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vhsSource |
VHSv20201209 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vhsSource |
VHSv20231101 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vhsSource |
VHSv20240731 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
videoSource |
VIDEODR2 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
videoSource |
VIDEODR3 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
videoSource |
VIDEODR4 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
videoSource |
VIDEODR5 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
videoSource |
VIDEOv20100513 |
Extended source Ks mag, no aperture correction applied |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
videoSource |
VIDEOv20111208 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vikingSource |
VIKINGDR2 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vikingSource |
VIKINGDR3 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vikingSource |
VIKINGDR4 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vikingSource |
VIKINGv20110714 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vikingSource |
VIKINGv20111019 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vikingSource |
VIKINGv20130417 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vikingSource |
VIKINGv20140402 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vikingSource |
VIKINGv20150421 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vikingSource |
VIKINGv20151230 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vikingSource |
VIKINGv20160406 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vikingSource |
VIKINGv20161202 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vikingSource |
VIKINGv20170715 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Point source Ks aperture corrected (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Point source Ks aperture corrected (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vmcSource |
VMCDR1 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vmcSource |
VMCDR2 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCDR3 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCDR4 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCDR5 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20110816 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vmcSource |
VMCv20110909 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vmcSource |
VMCv20120126 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vmcSource |
VMCv20121128 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vmcSource |
VMCv20130304 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMag6 |
vmcSource |
VMCv20130805 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20140428 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20140903 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20150309 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20151218 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20160311 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20160822 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20170109 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20170411 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20171101 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20180702 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20181120 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20191212 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20210708 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20230816 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcSource |
VMCv20240226 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcdeepSource |
VMCDEEPv20230713 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6 |
vmcdeepSource |
VMCDEEPv20240506 |
Point source Ks aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMag6Err |
sharksSource |
SHARKSv20210222 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
sharksSource |
SHARKSv20210421 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
ultravistaSource |
ULTRAVISTADR4 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Error in point/extended source Ks (5.7 arcsec aperture diameter) magnitude |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vhsSource |
VHSDR1 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vhsSource |
VHSDR2 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vhsSource |
VHSDR3 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag6Err |
vhsSource |
VHSDR4 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag6Err |
vhsSource |
VHSDR5 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vhsSource |
VHSDR6 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vhsSource |
VHSv20120926 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vhsSource |
VHSv20130417 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vhsSource |
VHSv20140409 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag6Err |
vhsSource |
VHSv20150108 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag6Err |
vhsSource |
VHSv20160114 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vhsSource |
VHSv20160507 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vhsSource |
VHSv20170630 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vhsSource |
VHSv20180419 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vhsSource |
VHSv20201209 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vhsSource |
VHSv20231101 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vhsSource |
VHSv20240731 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
videoSource |
VIDEODR2 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
videoSource |
VIDEODR3 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
videoSource |
VIDEODR4 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag6Err |
videoSource |
VIDEODR5 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag6Err |
videoSource |
VIDEOv20100513 |
Error in extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
videoSource |
VIDEOv20111208 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vikingSource |
VIKINGDR2 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vikingSource |
VIKINGDR3 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vikingSource |
VIKINGDR4 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag6Err |
vikingSource |
VIKINGv20110714 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vikingSource |
VIKINGv20111019 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vikingSource |
VIKINGv20130417 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vikingSource |
VIKINGv20140402 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vikingSource |
VIKINGv20150421 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag6Err |
vikingSource |
VIKINGv20151230 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vikingSource |
VIKINGv20160406 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vikingSource |
VIKINGv20161202 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vikingSource |
VIKINGv20170715 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Error in point/extended source Ks (5.7 arcsec aperture diameter) magnitude |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Error in point/extended source Ks (5.7 arcsec aperture diameter) magnitude |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vmcSource |
VMCDR1 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vmcSource |
VMCDR2 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vmcSource |
VMCDR3 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag6Err |
vmcSource |
VMCDR4 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCDR5 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20110816 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vmcSource |
VMCv20110909 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vmcSource |
VMCv20120126 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vmcSource |
VMCv20121128 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vmcSource |
VMCv20130304 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vmcSource |
VMCv20130805 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
ksAperMag6Err |
vmcSource |
VMCv20140428 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20140903 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag6Err |
vmcSource |
VMCv20150309 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.IR.K;phot.mag |
ksAperMag6Err |
vmcSource |
VMCv20151218 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20160311 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20160822 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20170109 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20170411 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20171101 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20180702 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20181120 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20191212 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20210708 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20230816 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcSource |
VMCv20240226 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcdeepSource |
VMCDEEPv20230713 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMag6Err |
vmcdeepSource |
VMCDEEPv20240506 |
Error in point/extended source Ks mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
sharksSource |
SHARKSv20210222 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
sharksSource |
SHARKSv20210421 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
ultravistaSource |
ULTRAVISTADR4 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Default extended source Ks (2.0 arcsec aperture diameter, but no aperture correction applied) aperture magnitude If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vhsSource |
VHSDR1 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vhsSource |
VHSDR2 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vhsSource |
VHSDR3 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vhsSource |
VHSDR4 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vhsSource |
VHSDR5 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vhsSource |
VHSDR6 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vhsSource |
VHSv20120926 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vhsSource |
VHSv20130417 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vhsSource |
VHSv20140409 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vhsSource |
VHSv20150108 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vhsSource |
VHSv20160114 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vhsSource |
VHSv20160507 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vhsSource |
VHSv20170630 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vhsSource |
VHSv20180419 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vhsSource |
VHSv20201209 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vhsSource |
VHSv20231101 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vhsSource |
VHSv20240731 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
videoSource |
VIDEODR2 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
videoSource |
VIDEODR3 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
videoSource |
VIDEODR4 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
videoSource |
VIDEODR5 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
videoSource |
VIDEOv20111208 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vikingSource |
VIKINGDR2 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vikingSource |
VIKINGDR3 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vikingSource |
VIKINGDR4 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vikingSource |
VIKINGv20110714 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vikingSource |
VIKINGv20111019 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vikingSource |
VIKINGv20130417 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vikingSource |
VIKINGv20140402 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vikingSource |
VIKINGv20150421 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vikingSource |
VIKINGv20151230 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vikingSource |
VIKINGv20160406 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vikingSource |
VIKINGv20161202 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vikingSource |
VIKINGv20170715 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Default extended source Ks (2.0 arcsec aperture diameter, but no aperture correction applied) aperture magnitude If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Default extended source Ks (2.0 arcsec aperture diameter, but no aperture correction applied) aperture magnitude If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vmcSource |
VMCDR1 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vmcSource |
VMCDR2 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCDR3 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCDR4 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCDR5 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20110816 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20110909 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20120126 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20121128 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20130304 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20130805 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20140428 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20140903 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20150309 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20151218 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20160311 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20160822 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20170109 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20170411 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20171101 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20180702 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20181120 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20191212 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20210708 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20230816 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcSource |
VMCv20240226 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcdeepSource |
VMCDEEPv20230713 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr3 |
vmcdeepSource |
VMCDEEPv20240506 |
Default extended source Ks aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
sharksSource |
SHARKSv20210222 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
sharksSource |
SHARKSv20210421 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
ultravistaSource |
ULTRAVISTADR4 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Extended source Ks (2.8 arcsec aperture diameter, but no aperture correction applied) aperture magnitude |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vhsSource |
VHSDR1 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vhsSource |
VHSDR2 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vhsSource |
VHSDR3 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vhsSource |
VHSDR4 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vhsSource |
VHSDR5 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vhsSource |
VHSDR6 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vhsSource |
VHSv20120926 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vhsSource |
VHSv20130417 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vhsSource |
VHSv20140409 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vhsSource |
VHSv20150108 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vhsSource |
VHSv20160114 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vhsSource |
VHSv20160507 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vhsSource |
VHSv20170630 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vhsSource |
VHSv20180419 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vhsSource |
VHSv20201209 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vhsSource |
VHSv20231101 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vhsSource |
VHSv20240731 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
videoSource |
VIDEODR2 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
videoSource |
VIDEODR3 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
videoSource |
VIDEODR4 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
videoSource |
VIDEODR5 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
videoSource |
VIDEOv20111208 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vikingSource |
VIKINGDR2 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vikingSource |
VIKINGDR3 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vikingSource |
VIKINGDR4 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vikingSource |
VIKINGv20110714 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vikingSource |
VIKINGv20111019 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vikingSource |
VIKINGv20130417 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vikingSource |
VIKINGv20140402 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vikingSource |
VIKINGv20150421 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vikingSource |
VIKINGv20151230 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vikingSource |
VIKINGv20160406 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vikingSource |
VIKINGv20161202 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vikingSource |
VIKINGv20170715 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Extended source Ks (2.8 arcsec aperture diameter, but no aperture correction applied) aperture magnitude |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Extended source Ks (2.8 arcsec aperture diameter, but no aperture correction applied) aperture magnitude |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vmcSource |
VMCDR1 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vmcSource |
VMCDR2 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCDR3 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCDR4 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCDR5 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20110816 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20110909 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20120126 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20121128 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20130304 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20130805 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20140428 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20140903 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20150309 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20151218 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20160311 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20160822 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20170109 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20170411 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20171101 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20180702 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20181120 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20191212 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20210708 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20230816 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcSource |
VMCv20240226 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcdeepSource |
VMCDEEPv20230713 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr4 |
vmcdeepSource |
VMCDEEPv20240506 |
Extended source Ks aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
sharksSource |
SHARKSv20210222 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
sharksSource |
SHARKSv20210421 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
ultravistaSource |
ULTRAVISTADR4 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
Extended source Ks (5.7 arcsec aperture diameter, but no aperture correction applied) aperture magnitude |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vhsSource |
VHSDR1 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vhsSource |
VHSDR2 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vhsSource |
VHSDR3 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vhsSource |
VHSDR4 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vhsSource |
VHSDR5 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vhsSource |
VHSDR6 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vhsSource |
VHSv20120926 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vhsSource |
VHSv20130417 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vhsSource |
VHSv20140409 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vhsSource |
VHSv20150108 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vhsSource |
VHSv20160114 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vhsSource |
VHSv20160507 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vhsSource |
VHSv20170630 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vhsSource |
VHSv20180419 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vhsSource |
VHSv20201209 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vhsSource |
VHSv20231101 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vhsSource |
VHSv20240731 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
videoSource |
VIDEODR2 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
videoSource |
VIDEODR3 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
videoSource |
VIDEODR4 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
videoSource |
VIDEODR5 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
videoSource |
VIDEOv20111208 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vikingSource |
VIKINGDR2 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vikingSource |
VIKINGDR3 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vikingSource |
VIKINGDR4 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vikingSource |
VIKINGv20110714 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vikingSource |
VIKINGv20111019 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vikingSource |
VIKINGv20130417 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vikingSource |
VIKINGv20140402 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vikingSource |
VIKINGv20150421 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vikingSource |
VIKINGv20151230 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vikingSource |
VIKINGv20160406 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vikingSource |
VIKINGv20161202 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vikingSource |
VIKINGv20170715 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
Extended source Ks (5.7 arcsec aperture diameter, but no aperture correction applied) aperture magnitude |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
Extended source Ks (5.7 arcsec aperture diameter, but no aperture correction applied) aperture magnitude |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vmcSource |
VMCDR1 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vmcSource |
VMCDR2 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCDR3 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCDR4 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCDR5 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20110816 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20110909 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20120126 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20121128 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20130304 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20130805 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20140428 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20140903 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20150309 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20151218 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20160311 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20160822 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20170109 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20170411 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20171101 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20180702 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20181120 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20191212 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20210708 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20230816 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcSource |
VMCv20240226 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcdeepSource |
VMCDEEPv20230713 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksAperMagNoAperCorr6 |
vmcdeepSource |
VMCDEEPv20240506 |
Extended source Ks aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.IR.K |
ksaStratAst |
sharksVarFrameSetInfo |
SHARKSv20210222 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
sharksVarFrameSetInfo |
SHARKSv20210421 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
ultravistaVarFrameSetInfo |
ULTRAVISTADR4 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
videoVarFrameSetInfo |
VIDEODR2 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
videoVarFrameSetInfo |
VIDEODR3 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
videoVarFrameSetInfo |
VIDEODR4 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
videoVarFrameSetInfo |
VIDEODR5 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
videoVarFrameSetInfo |
VIDEOv20100513 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
videoVarFrameSetInfo |
VIDEOv20111208 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vikingVarFrameSetInfo |
VIKINGDR2 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vikingVarFrameSetInfo |
VIKINGv20110714 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vikingVarFrameSetInfo |
VIKINGv20111019 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCDR1 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCDR2 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCDR3 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCDR4 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCDR5 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20110816 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20110909 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20120126 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20121128 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20130304 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20130805 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20140428 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20140903 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20150309 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20151218 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20160311 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20160822 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20170109 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20170411 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20171101 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20180702 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20181120 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20191212 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20210708 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20230816 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcVarFrameSetInfo |
VMCv20240226 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcdeepVarFrameSetInfo |
VMCDEEPv20230713 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vmcdeepVarFrameSetInfo |
VMCDEEPv20240506 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vvvVarFrameSetInfo |
VVVDR1 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vvvVarFrameSetInfo |
VVVDR2 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vvvVarFrameSetInfo |
VVVDR5 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vvvVarFrameSetInfo |
VVVv20100531 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratAst |
vvvVarFrameSetInfo |
VVVv20110718 |
Strateva parameter, a, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksaStratPht |
sharksVarFrameSetInfo |
SHARKSv20210222 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
sharksVarFrameSetInfo |
SHARKSv20210421 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
ultravistaMapLcVarFrameSetInfo |
ULTRAVISTADR4 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
ultravistaVarFrameSetInfo |
ULTRAVISTADR4 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
videoVarFrameSetInfo |
VIDEODR2 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
videoVarFrameSetInfo |
VIDEODR3 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
videoVarFrameSetInfo |
VIDEODR4 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
videoVarFrameSetInfo |
VIDEODR5 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
videoVarFrameSetInfo |
VIDEOv20100513 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
videoVarFrameSetInfo |
VIDEOv20111208 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vikingVarFrameSetInfo |
VIKINGDR2 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vikingVarFrameSetInfo |
VIKINGv20110714 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vikingVarFrameSetInfo |
VIKINGv20111019 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCDR1 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCDR2 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCDR3 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCDR4 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCDR5 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20110816 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20110909 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20120126 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20121128 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20130304 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20130805 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20140428 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20140903 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20150309 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20151218 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20160311 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20160822 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20170109 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20170411 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20171101 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20180702 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20181120 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20191212 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20210708 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20230816 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcVarFrameSetInfo |
VMCv20240226 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcdeepVarFrameSetInfo |
VMCDEEPv20230713 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vmcdeepVarFrameSetInfo |
VMCDEEPv20240506 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vvvVarFrameSetInfo |
VVVDR1 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vvvVarFrameSetInfo |
VVVDR2 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vvvVarFrameSetInfo |
VVVDR5 |
Parameter, c0 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vvvVarFrameSetInfo |
VVVv20100531 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksaStratPht |
vvvVarFrameSetInfo |
VVVv20110718 |
Strateva parameter, a, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksAverageConf |
sharksSource |
SHARKSv20210222 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
sharksSource |
SHARKSv20210421 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vhsSource |
VHSDR1 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
meta.code |
ksAverageConf |
vhsSource |
VHSDR2 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
meta.code |
ksAverageConf |
vhsSource |
VHSDR3 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vhsSource |
VHSDR4 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vhsSource |
VHSDR5 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vhsSource |
VHSDR6 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vhsSource |
VHSv20120926 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vhsSource |
VHSv20130417 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vhsSource |
VHSv20140409 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vhsSource |
VHSv20150108 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vhsSource |
VHSv20160114 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vhsSource |
VHSv20160507 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vhsSource |
VHSv20170630 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vhsSource |
VHSv20180419 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vhsSource |
VHSv20201209 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vhsSource |
VHSv20231101 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vhsSource |
VHSv20240731 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vikingSource |
VIKINGDR2 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
meta.code |
ksAverageConf |
vikingSource |
VIKINGDR3 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vikingSource |
VIKINGDR4 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vikingSource |
VIKINGv20110714 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
meta.code |
ksAverageConf |
vikingSource |
VIKINGv20111019 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
meta.code |
ksAverageConf |
vikingSource |
VIKINGv20130417 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vikingSource |
VIKINGv20140402 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vikingSource |
VIKINGv20150421 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vikingSource |
VIKINGv20151230 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vikingSource |
VIKINGv20160406 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vikingSource |
VIKINGv20161202 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vikingSource |
VIKINGv20170715 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vmcSource |
VMCDR2 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vmcSource |
VMCDR3 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCDR4 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCDR5 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20110816 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
meta.code |
ksAverageConf |
vmcSource |
VMCv20110909 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
meta.code |
ksAverageConf |
vmcSource |
VMCv20120126 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
meta.code |
ksAverageConf |
vmcSource |
VMCv20121128 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vmcSource |
VMCv20130304 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vmcSource |
VMCv20130805 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vmcSource |
VMCv20140428 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20140903 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20150309 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20151218 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20160311 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20160822 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20170109 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20170411 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20171101 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20180702 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20181120 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20191212 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20210708 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20230816 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource |
VMCv20240226 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcSource, vmcSynopticSource |
VMCDR1 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
meta.code |
ksAverageConf |
vmcdeepSource |
VMCDEEPv20240506 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vmcdeepSource, vmcdeepSynopticSource |
VMCDEEPv20230713 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vvvSource |
VVVDR2 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.NIR |
ksAverageConf |
vvvSource |
VVVDR5 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-0.9999995e9 |
stat.likelihood;em.IR.K |
ksAverageConf |
vvvSource, vvvSynopticSource |
VVVDR1 |
average confidence in 2 arcsec diameter default aperture (aper3) Ks |
real |
4 |
|
-99999999 |
stat.likelihood;em.IR.NIR |
ksbestAper |
sharksVariability |
SHARKSv20210222 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
sharksVariability |
SHARKSv20210421 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
ultravistaMapLcVariability |
ULTRAVISTADR4 |
Best aperture (1-3) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
ultravistaVariability |
ULTRAVISTADR4 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
videoVariability |
VIDEODR2 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
videoVariability |
VIDEODR3 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.NIR |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
videoVariability |
VIDEODR4 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
videoVariability |
VIDEODR5 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
videoVariability |
VIDEOv20100513 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
videoVariability |
VIDEOv20111208 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vikingVariability |
VIKINGDR2 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vikingVariability |
VIKINGv20110714 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vikingVariability |
VIKINGv20111019 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCDR1 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCDR2 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.NIR |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCDR3 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCDR4 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCDR5 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20110816 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20110909 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20120126 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20121128 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.NIR |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20130304 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.NIR |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20130805 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.NIR |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20140428 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20140903 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20150309 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20151218 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20160311 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20160822 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20170109 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20170411 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20171101 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20180702 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20181120 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20191212 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20210708 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20230816 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcVariability |
VMCv20240226 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcdeepVariability |
VMCDEEPv20230713 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vmcdeepVariability |
VMCDEEPv20240506 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vvvVariability |
VVVDR1 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.NIR |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vvvVariability |
VVVDR2 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.NIR |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vvvVariability |
VVVDR5 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
meta.code.class;em.IR.K |
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vvvVariability |
VVVv20100531 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbestAper |
vvvVariability |
VVVv20110718 |
Best aperture (1-6) for photometric statistics in the Ks band |
int |
4 |
|
-9999 |
|
Aperture magnitude (1-6) which gives the lowest RMS for the object. All apertures have the appropriate aperture correction. This can give better values in crowded regions than aperMag3 (see Irwin et al. 2007, MNRAS, 375, 1449) |
ksbStratAst |
sharksVarFrameSetInfo |
SHARKSv20210222 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
sharksVarFrameSetInfo |
SHARKSv20210421 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
ultravistaVarFrameSetInfo |
ULTRAVISTADR4 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
videoVarFrameSetInfo |
VIDEODR2 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
videoVarFrameSetInfo |
VIDEODR3 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
videoVarFrameSetInfo |
VIDEODR4 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
videoVarFrameSetInfo |
VIDEODR5 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
videoVarFrameSetInfo |
VIDEOv20100513 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
videoVarFrameSetInfo |
VIDEOv20111208 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vikingVarFrameSetInfo |
VIKINGDR2 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vikingVarFrameSetInfo |
VIKINGv20110714 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vikingVarFrameSetInfo |
VIKINGv20111019 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCDR1 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCDR2 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCDR3 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCDR4 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCDR5 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20110816 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20110909 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20120126 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20121128 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20130304 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20130805 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20140428 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20140903 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20150309 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20151218 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20160311 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20160822 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20170109 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20170411 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20171101 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20180702 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20181120 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20191212 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20210708 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20230816 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcVarFrameSetInfo |
VMCv20240226 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcdeepVarFrameSetInfo |
VMCDEEPv20230713 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vmcdeepVarFrameSetInfo |
VMCDEEPv20240506 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vvvVarFrameSetInfo |
VVVDR1 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vvvVarFrameSetInfo |
VVVDR2 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vvvVarFrameSetInfo |
VVVDR5 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vvvVarFrameSetInfo |
VVVv20100531 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratAst |
vvvVarFrameSetInfo |
VVVv20110718 |
Strateva parameter, b, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
ksbStratPht |
sharksVarFrameSetInfo |
SHARKSv20210222 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
sharksVarFrameSetInfo |
SHARKSv20210421 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
ultravistaMapLcVarFrameSetInfo |
ULTRAVISTADR4 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
ultravistaVarFrameSetInfo |
ULTRAVISTADR4 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
videoVarFrameSetInfo |
VIDEODR2 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
videoVarFrameSetInfo |
VIDEODR3 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
videoVarFrameSetInfo |
VIDEODR4 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
videoVarFrameSetInfo |
VIDEODR5 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
videoVarFrameSetInfo |
VIDEOv20100513 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
videoVarFrameSetInfo |
VIDEOv20111208 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vikingVarFrameSetInfo |
VIKINGDR2 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vikingVarFrameSetInfo |
VIKINGv20110714 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vikingVarFrameSetInfo |
VIKINGv20111019 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCDR1 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCDR2 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCDR3 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCDR4 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCDR5 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20110816 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20110909 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20120126 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20121128 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20130304 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20130805 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20140428 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20140903 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20150309 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20151218 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20160311 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20160822 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20170109 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20170411 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20171101 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20180702 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20181120 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20191212 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20210708 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20230816 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcVarFrameSetInfo |
VMCv20240226 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcdeepVarFrameSetInfo |
VMCDEEPv20230713 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vmcdeepVarFrameSetInfo |
VMCDEEPv20240506 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vvvVarFrameSetInfo |
VVVDR1 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vvvVarFrameSetInfo |
VVVDR2 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vvvVarFrameSetInfo |
VVVDR5 |
Parameter, c1 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to photometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vvvVarFrameSetInfo |
VVVv20100531 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksbStratPht |
vvvVarFrameSetInfo |
VVVv20110718 |
Strateva parameter, b, in fit to photometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqAst |
sharksVarFrameSetInfo |
SHARKSv20210222 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
sharksVarFrameSetInfo |
SHARKSv20210421 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
ultravistaVarFrameSetInfo |
ULTRAVISTADR4 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
videoVarFrameSetInfo |
VIDEODR2 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
videoVarFrameSetInfo |
VIDEODR3 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
videoVarFrameSetInfo |
VIDEODR4 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
videoVarFrameSetInfo |
VIDEODR5 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
videoVarFrameSetInfo |
VIDEOv20100513 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
videoVarFrameSetInfo |
VIDEOv20111208 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vikingVarFrameSetInfo |
VIKINGDR2 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vikingVarFrameSetInfo |
VIKINGv20110714 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vikingVarFrameSetInfo |
VIKINGv20111019 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCDR1 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCDR2 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCDR3 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCDR4 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCDR5 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20110816 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20110909 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20120126 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20121128 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20130304 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20130805 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20140428 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20140903 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20150309 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20151218 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20160311 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20160822 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20170109 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20170411 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20171101 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20180702 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20181120 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20191212 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20210708 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20230816 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcVarFrameSetInfo |
VMCv20240226 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcdeepVarFrameSetInfo |
VMCDEEPv20230713 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vmcdeepVarFrameSetInfo |
VMCDEEPv20240506 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vvvVarFrameSetInfo |
VVVDR1 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vvvVarFrameSetInfo |
VVVDR2 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vvvVarFrameSetInfo |
VVVDR5 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vvvVarFrameSetInfo |
VVVv20100531 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqAst |
vvvVarFrameSetInfo |
VVVv20110718 |
Goodness of fit of Strateva function to astrometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kschiSqpd |
sharksVariability |
SHARKSv20210222 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
sharksVariability |
SHARKSv20210421 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
ultravistaMapLcVariability |
ULTRAVISTADR4 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
ultravistaVariability |
ULTRAVISTADR4 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
videoVariability |
VIDEODR2 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
videoVariability |
VIDEODR3 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2 |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
videoVariability |
VIDEODR4 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
videoVariability |
VIDEODR5 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
videoVariability |
VIDEOv20100513 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
videoVariability |
VIDEOv20111208 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vikingVariability |
VIKINGDR2 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vikingVariability |
VIKINGv20110714 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vikingVariability |
VIKINGv20111019 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCDR1 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCDR2 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2 |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCDR3 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCDR4 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCDR5 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20110816 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20110909 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20120126 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20121128 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2 |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20130304 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2 |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20130805 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2 |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20140428 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20140903 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20150309 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20151218 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20160311 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20160822 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20170109 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20170411 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20171101 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20180702 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20181120 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20191212 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20210708 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20230816 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcVariability |
VMCv20240226 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcdeepVariability |
VMCDEEPv20230713 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vmcdeepVariability |
VMCDEEPv20240506 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vvvVariability |
VVVDR1 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2 |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vvvVariability |
VVVDR2 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2 |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vvvVariability |
VVVDR5 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
stat.fit.chi2;em.IR.K |
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vvvVariability |
VVVv20100531 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqpd |
vvvVariability |
VVVv20110718 |
Chi square (per degree of freedom) fit to data (mean and expected rms) |
real |
4 |
|
-0.9999995e9 |
|
The photometry is calculated for good observations in the best aperture. The mean, rms, median, median absolute deviation, minMag and maxMag are quite standard. The skewness is calculated as in Sesar et al. 2007, AJ, 134, 2236. The number of good detections that are more than 3 standard deviations can indicate a distribution with many outliers. In each frameset, the mean and rms are used to derive a fit to the expected rms as a function of magnitude. The parameters for the fit are stored in VarFrameSetInfo and the value for the source is in expRms. This is subtracted from the rms in quadrature to get the intrinsic rms: the variability of the object beyond the noise in the system. The chi-squared is calculated, assuming a non-variable object which has the noise from the expected-rms and mean calculated as above. The probVar statistic assumes a chi-squared distribution with the correct number of degrees of freedom. The varClass statistic is 1, if the probVar>0.9 and intrinsicRMS/expectedRMS>3. |
kschiSqPht |
sharksVarFrameSetInfo |
SHARKSv20210222 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
sharksVarFrameSetInfo |
SHARKSv20210421 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
ultravistaMapLcVarFrameSetInfo, ultravistaVarFrameSetInfo |
ULTRAVISTADR4 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
videoVarFrameSetInfo |
VIDEODR2 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
videoVarFrameSetInfo |
VIDEODR3 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
videoVarFrameSetInfo |
VIDEODR4 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
videoVarFrameSetInfo |
VIDEODR5 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
videoVarFrameSetInfo |
VIDEOv20100513 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
videoVarFrameSetInfo |
VIDEOv20111208 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vikingVarFrameSetInfo |
VIKINGDR2 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vikingVarFrameSetInfo |
VIKINGv20110714 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vikingVarFrameSetInfo |
VIKINGv20111019 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCDR1 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCDR2 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCDR3 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCDR4 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCDR5 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20110816 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20110909 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20120126 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20121128 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20130304 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20130805 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20140428 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20140903 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20150309 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20151218 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20160311 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20160822 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20170109 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20170411 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20171101 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20180702 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20181120 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20191212 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20210708 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20230816 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcVarFrameSetInfo |
VMCv20240226 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcdeepVarFrameSetInfo |
VMCDEEPv20230713 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vmcdeepVarFrameSetInfo |
VMCDEEPv20240506 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vvvVarFrameSetInfo |
VVVDR1 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vvvVarFrameSetInfo |
VVVDR2 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.NIR |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vvvVarFrameSetInfo |
VVVDR5 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
stat.fit.goodness;em.IR.K |
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vvvVarFrameSetInfo |
VVVv20100531 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
kschiSqPht |
vvvVarFrameSetInfo |
VVVv20110718 |
Goodness of fit of Strateva function to photometric data in Ks band |
real |
4 |
|
-0.9999995e9 |
|
The best fit solution to the expected RMS brightness (in magnitudes) for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. This technique was used in Sesar et al. 2007, AJ, 134, 2236. |
ksClass |
sharksSource |
SHARKSv20210222 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
sharksSource |
SHARKSv20210421 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
ultravistaSource |
ULTRAVISTADR4 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vhsSource |
VHSDR2 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vhsSource |
VHSDR3 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource |
VHSDR4 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource |
VHSDR5 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource |
VHSDR6 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource |
VHSv20120926 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vhsSource |
VHSv20130417 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vhsSource |
VHSv20140409 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource |
VHSv20150108 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource |
VHSv20160114 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource |
VHSv20160507 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource |
VHSv20170630 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource |
VHSv20180419 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource |
VHSv20201209 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource |
VHSv20231101 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource |
VHSv20240731 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vhsSource, vhsSourceRemeasurement |
VHSDR1 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
videoSource |
VIDEODR2 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
videoSource |
VIDEODR3 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
videoSource |
VIDEODR4 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
videoSource |
VIDEODR5 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
videoSource |
VIDEOv20111208 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
videoSource, videoSourceRemeasurement |
VIDEOv20100513 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vikingSource |
VIKINGDR2 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vikingSource |
VIKINGDR3 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vikingSource |
VIKINGDR4 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vikingSource |
VIKINGv20111019 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vikingSource |
VIKINGv20130417 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vikingSource |
VIKINGv20140402 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vikingSource |
VIKINGv20150421 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vikingSource |
VIKINGv20151230 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vikingSource |
VIKINGv20160406 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vikingSource |
VIKINGv20161202 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vikingSource |
VIKINGv20170715 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vikingSource, vikingSourceRemeasurement |
VIKINGv20110714 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vmcSource |
VMCDR2 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vmcSource |
VMCDR3 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCDR4 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCDR5 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20110909 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vmcSource |
VMCv20120126 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vmcSource |
VMCv20121128 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vmcSource |
VMCv20130304 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vmcSource |
VMCv20130805 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vmcSource |
VMCv20140428 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20140903 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20150309 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20151218 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20160311 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20160822 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20170109 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20170411 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20171101 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20180702 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20181120 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20191212 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20210708 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20230816 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource |
VMCv20240226 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcSource, vmcSourceRemeasurement |
VMCv20110816 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vmcSource, vmcSynopticSource |
VMCDR1 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vmcdeepSource |
VMCDEEPv20240506 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vmcdeepSource, vmcdeepSynopticSource |
VMCDEEPv20230713 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vvvSource |
VVVDR2 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vvvSource |
VVVDR5 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class;em.IR.K |
ksClass |
vvvSource |
VVVv20110718 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vvvSource, vvvSourceRemeasurement |
VVVv20100531 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClass |
vvvSource, vvvSynopticSource |
VVVDR1 |
discrete image classification flag in Ks |
smallint |
2 |
|
-9999 |
src.class |
ksClassStat |
sharksSource |
SHARKSv20210222 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
sharksSource |
SHARKSv20210421 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
ultravistaSource |
ULTRAVISTADR4 |
S-Extractor classification statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
ultravistaSourceRemeasurement |
ULTRAVISTADR4 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vhsSource |
VHSDR2 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vhsSource |
VHSDR3 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource |
VHSDR4 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource |
VHSDR5 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource |
VHSDR6 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource |
VHSv20120926 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vhsSource |
VHSv20130417 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vhsSource |
VHSv20140409 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource |
VHSv20150108 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource |
VHSv20160114 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource |
VHSv20160507 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource |
VHSv20170630 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource |
VHSv20180419 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource |
VHSv20201209 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource |
VHSv20231101 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource |
VHSv20240731 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vhsSource, vhsSourceRemeasurement |
VHSDR1 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
videoSource |
VIDEODR2 |
S-Extractor classification statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
videoSource |
VIDEODR3 |
S-Extractor classification statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
videoSource |
VIDEODR4 |
S-Extractor classification statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
videoSource |
VIDEODR5 |
S-Extractor classification statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
videoSource |
VIDEOv20100513 |
S-Extractor classification statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
videoSource |
VIDEOv20111208 |
S-Extractor classification statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
videoSourceRemeasurement |
VIDEOv20100513 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vikingSource |
VIKINGDR2 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vikingSource |
VIKINGDR3 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vikingSource |
VIKINGDR4 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vikingSource |
VIKINGv20111019 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vikingSource |
VIKINGv20130417 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vikingSource |
VIKINGv20140402 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vikingSource |
VIKINGv20150421 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vikingSource |
VIKINGv20151230 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vikingSource |
VIKINGv20160406 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vikingSource |
VIKINGv20161202 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vikingSource |
VIKINGv20170715 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vikingSource, vikingSourceRemeasurement |
VIKINGv20110714 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20160909 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vikingZY_selJ_SourceRemeasurement |
VIKINGZYSELJv20170124 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vmcSource |
VMCDR2 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vmcSource |
VMCDR3 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCDR4 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCDR5 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20110909 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vmcSource |
VMCv20120126 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vmcSource |
VMCv20121128 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vmcSource |
VMCv20130304 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vmcSource |
VMCv20130805 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vmcSource |
VMCv20140428 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20140903 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20150309 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20151218 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20160311 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20160822 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20170109 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20170411 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20171101 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20180702 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20181120 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20191212 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20210708 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20230816 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource |
VMCv20240226 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcSource, vmcSourceRemeasurement |
VMCv20110816 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vmcSource, vmcSynopticSource |
VMCDR1 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vmcdeepSource |
VMCDEEPv20240506 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vmcdeepSource, vmcdeepSynopticSource |
VMCDEEPv20230713 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vvvSource |
VVVDR1 |
S-Extractor classification statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vvvSource |
VVVDR2 |
S-Extractor classification statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vvvSource |
VVVDR5 |
S-Extractor classification statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat;em.IR.K |
ksClassStat |
vvvSource |
VVVv20100531 |
S-Extractor classification statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vvvSource |
VVVv20110718 |
S-Extractor classification statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vvvSourceRemeasurement |
VVVv20100531 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vvvSourceRemeasurement |
VVVv20110718 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vvvSynopticSource |
VVVDR1 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
ksClassStat |
vvvSynopticSource |
VVVDR2 |
N(0,1) stellarness-of-profile statistic in Ks |
real |
4 |
|
-0.9999995e9 |
stat |
kscStratAst |
sharksVarFrameSetInfo |
SHARKSv20210222 |
Parameter, c2 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kscStratAst |
sharksVarFrameSetInfo |
SHARKSv20210421 |
Parameter, c2 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kscStratAst |
ultravistaVarFrameSetInfo |
ULTRAVISTADR4 |
Parameter, c2 from Ferreira-Lopes & Cross 2017, Eq. 18, in fit to astrometric rms vs magnitude in Ks band. |
real |
4 |
|
-0.9999995e9 |
stat.fit.param;em.IR.K |
The best fit solution to the expected RMS position around the mean for all objects in the frameset. Objects were binned in ranges of magnitude and the median RMS (after clipping out variable objects using the median-absolute deviation) was calculated. The Strateva function $\zeta(m)>=a+b\,10^{0.4m}+c\,10^{0.8m}$ was fit, where $\zeta(m)$ is the expected RMS as a function of magnitude. The chi-squared and number of degrees of freedom are also calculated. |
kscStratAst |
videoVarFrameSetInfo |
VIDEODR2 |
Strateva parameter, c, in fit to astrometric rms vs magnitude in Ks band, see Sesar et al. 2007. |
real |
4 |
|
-0.9999995e9 |
|
|