G |
Name | Schema Table | Database | Description | Type | Length | Unit | Default Value | Unified Content Descriptor |
g_flux |
phot_variable_time_series_g_fov |
GAIADR1 |
G-band flux for each FoV observation |
float |
8 |
electrons/second |
|
phot.flux;em.opt |
g_flux_error |
phot_variable_time_series_g_fov |
GAIADR1 |
Estimated uncertainty on G-band flux for each FoV observation |
float |
8 |
electrons/second |
|
stat.error;phot.flux;em.opt |
g_mag_zero_oint_error |
ext_phot_zero_point |
GAIADR1 |
Uncertainty on G magnitude zero point |
float |
8 |
mag |
|
stat.error;phot.mag;arith.zp;em.opt |
g_mag_zero_point |
ext_phot_zero_point |
GAIADR1 |
G magnitude zero point |
float |
8 |
mag |
|
phot.mag;arith.zp;em.opt |
g_magnitude |
phot_variable_time_series_g_fov |
GAIADR1 |
G-band magnitude for each FoV observation |
float |
8 |
mag |
|
phot.mag;em.opt |
g_rp |
gaia_source |
GAIADR2 |
G-RP colour |
real |
4 |
mag |
|
phot.colour |
g_score |
twomass_xsc |
TWOMASS |
galaxy score: 1(extended) < g_score < 2(point-like). |
real |
4 |
|
|
meta.code |
gainCor |
MultiframeDetector |
ATLASDR1 |
Gain correction factor {image extension keyword: GAINCOR} |
real |
4 |
|
-9.999995e+08 |
|
gainCor |
MultiframeDetector |
ATLASDR2 |
Gain correction factor {image extension keyword: GAINCOR} |
real |
4 |
|
-9.999995e+08 |
|
gainCor |
MultiframeDetector |
ATLASDR3 |
Gain correction factor {image extension keyword: GAINCOR} |
real |
4 |
|
-9.999995e+08 |
|
gainCor |
MultiframeDetector |
ATLASDR4 |
Gain correction factor {image extension keyword: GAINCOR} |
real |
4 |
|
-9.999995e+08 |
|
gainCor |
MultiframeDetector |
ATLASDR5 |
Gain correction factor {image extension keyword: GAINCOR} |
real |
4 |
|
-9.999995e+08 |
|
gainCor |
MultiframeDetector |
ATLASv20131127 |
Gain correction factor {image extension keyword: GAINCOR} |
real |
4 |
|
-9.999995e+08 |
|
gainCor |
MultiframeDetector |
ATLASv20160425 |
Gain correction factor {image extension keyword: GAINCOR} |
real |
4 |
|
-9.999995e+08 |
|
gainCor |
MultiframeDetector |
ATLASv20180209 |
Gain correction factor {image extension keyword: GAINCOR} |
real |
4 |
|
-9.999995e+08 |
|
gainCor |
MultiframeDetector |
VPHASDR3 |
Gain correction factor {image extension keyword: GAINCOR} |
real |
4 |
|
-9.999995e+08 |
|
gainCor |
MultiframeDetector |
VPHASv20160112 |
Gain correction factor {image extension keyword: GAINCOR} |
real |
4 |
|
-9.999995e+08 |
|
gainCor |
MultiframeDetector |
VPHASv20170222 |
Gain correction factor {image extension keyword: GAINCOR} |
real |
4 |
|
-9.999995e+08 |
|
gal_contam |
twomass_psc |
TWOMASS |
Extended source "contamination" flag. |
smallint |
2 |
|
|
meta.code |
gal_contam |
twomass_sixx2_psc |
TWOMASS |
src contaminated by galaxy (check blanked/subtracted tbl) |
smallint |
2 |
|
|
|
galactic_lat |
igsl_source |
GAIADR1 |
Galactic latitude |
real |
4 |
degrees |
|
pos.galatic.lat |
galactic_lon |
igsl_source |
GAIADR1 |
Galactic longitude |
real |
4 |
degrees |
|
pos.galatic.lon |
gAperMag3 |
atlasSource |
ATLASDR1 |
Default point source G aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMag3 |
atlasSource |
ATLASDR2 |
Default point source G aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMag3 |
atlasSource |
ATLASDR3 |
Default point source G aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag3 |
atlasSource |
ATLASDR4 |
Default point source G aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag3 |
atlasSource |
ATLASDR5 |
Default point source G aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag3 |
atlasSource |
ATLASv20131127 |
Default point source G aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMag3 |
atlasSource |
ATLASv20160425 |
Default point source G aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag3 |
atlasSource |
ATLASv20180209 |
Default point source G aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag3 |
vphasSource |
VPHASDR3 |
Default point source G aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag3 |
vphasSource |
VPHASv20160112 |
Default point source G aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag3 |
vphasSource |
VPHASv20170222 |
Default point source G aperture corrected mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag3Err |
atlasSource |
ATLASDR1 |
Error in default point/extended source G mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gAperMag3Err |
atlasSource |
ATLASDR2 |
Error in default point/extended source G mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gAperMag3Err |
atlasSource |
ATLASDR3 |
Error in default point/extended source G mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag3Err |
atlasSource |
ATLASDR4 |
Error in default point/extended source G mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag3Err |
atlasSource |
ATLASDR5 |
Error in default point/extended source G mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag3Err |
atlasSource |
ATLASv20131127 |
Error in default point/extended source G mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gAperMag3Err |
atlasSource |
ATLASv20160425 |
Error in default point/extended source G mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag3Err |
atlasSource |
ATLASv20180209 |
Error in default point/extended source G mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag3Err |
vphasSource |
VPHASDR3 |
Error in default point/extended source G mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag3Err |
vphasSource |
VPHASv20160112 |
Error in default point/extended source G mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag3Err |
vphasSource |
VPHASv20170222 |
Error in default point/extended source G mag (2.0 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag4 |
atlasSource |
ATLASDR1 |
Point source G aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMag4 |
atlasSource |
ATLASDR2 |
Point source G aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMag4 |
atlasSource |
ATLASDR3 |
Point source G aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag4 |
atlasSource |
ATLASDR4 |
Point source G aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag4 |
atlasSource |
ATLASDR5 |
Point source G aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag4 |
atlasSource |
ATLASv20131127 |
Point source G aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMag4 |
atlasSource |
ATLASv20160425 |
Point source G aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag4 |
atlasSource |
ATLASv20180209 |
Point source G aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag4 |
vphasSource |
VPHASDR3 |
Point source G aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag4 |
vphasSource |
VPHASv20160112 |
Point source G aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag4 |
vphasSource |
VPHASv20170222 |
Point source G aperture corrected mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag4Err |
atlasSource |
ATLASDR1 |
Error in point/extended source G mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gAperMag4Err |
atlasSource |
ATLASDR2 |
Error in point/extended source G mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gAperMag4Err |
atlasSource |
ATLASDR3 |
Error in point/extended source G mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag4Err |
atlasSource |
ATLASDR4 |
Error in point/extended source G mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag4Err |
atlasSource |
ATLASDR5 |
Error in point/extended source G mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag4Err |
atlasSource |
ATLASv20131127 |
Error in point/extended source G mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gAperMag4Err |
atlasSource |
ATLASv20160425 |
Error in point/extended source G mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag4Err |
atlasSource |
ATLASv20180209 |
Error in point/extended source G mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag4Err |
vphasSource |
VPHASDR3 |
Error in point/extended source G mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag4Err |
vphasSource |
VPHASv20160112 |
Error in point/extended source G mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag4Err |
vphasSource |
VPHASv20170222 |
Error in point/extended source G mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag6 |
atlasSource |
ATLASDR1 |
Point source G aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMag6 |
atlasSource |
ATLASDR2 |
Point source G aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMag6 |
atlasSource |
ATLASDR3 |
Point source G aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag6 |
atlasSource |
ATLASDR4 |
Point source G aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag6 |
atlasSource |
ATLASDR5 |
Point source G aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag6 |
atlasSource |
ATLASv20131127 |
Point source G aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMag6 |
atlasSource |
ATLASv20160425 |
Point source G aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag6 |
atlasSource |
ATLASv20180209 |
Point source G aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag6 |
vphasSource |
VPHASDR3 |
Point source G aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag6 |
vphasSource |
VPHASv20160112 |
Point source G aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag6 |
vphasSource |
VPHASv20170222 |
Point source G aperture corrected mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMag6Err |
atlasSource |
ATLASDR1 |
Error in point/extended source G mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gAperMag6Err |
atlasSource |
ATLASDR2 |
Error in point/extended source G mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gAperMag6Err |
atlasSource |
ATLASDR3 |
Error in point/extended source G mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag6Err |
atlasSource |
ATLASDR4 |
Error in point/extended source G mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag6Err |
atlasSource |
ATLASDR5 |
Error in point/extended source G mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag6Err |
atlasSource |
ATLASv20131127 |
Error in point/extended source G mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gAperMag6Err |
atlasSource |
ATLASv20160425 |
Error in point/extended source G mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag6Err |
atlasSource |
ATLASv20180209 |
Error in point/extended source G mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag6Err |
vphasSource |
VPHASDR3 |
Error in point/extended source G mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag6Err |
vphasSource |
VPHASv20160112 |
Error in point/extended source G mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMag6Err |
vphasSource |
VPHASv20170222 |
Error in point/extended source G mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gAperMagNoAperCorr3 |
atlasSource |
ATLASDR1 |
Default extended source G aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMagNoAperCorr3 |
atlasSource |
ATLASDR2 |
Default extended source G aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMagNoAperCorr3 |
atlasSource |
ATLASDR3 |
Default extended source G aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr3 |
atlasSource |
ATLASDR4 |
Default extended source G aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr3 |
atlasSource |
ATLASDR5 |
Default extended source G aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr3 |
atlasSource |
ATLASv20131127 |
Default extended source G aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMagNoAperCorr3 |
atlasSource |
ATLASv20160425 |
Default extended source G aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr3 |
atlasSource |
ATLASv20180209 |
Default extended source G aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr3 |
vphasSource |
VPHASDR3 |
Default extended source G aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr3 |
vphasSource |
VPHASv20160112 |
Default extended source G aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr3 |
vphasSource |
VPHASv20170222 |
Default extended source G aperture mag (2.0 arcsec aperture diameter) If in doubt use this flux estimator |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr4 |
atlasSource |
ATLASDR1 |
Extended source G aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMagNoAperCorr4 |
atlasSource |
ATLASDR2 |
Extended source G aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMagNoAperCorr4 |
atlasSource |
ATLASDR3 |
Extended source G aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr4 |
atlasSource |
ATLASDR4 |
Extended source G aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr4 |
atlasSource |
ATLASDR5 |
Extended source G aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr4 |
atlasSource |
ATLASv20131127 |
Extended source G aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMagNoAperCorr4 |
atlasSource |
ATLASv20160425 |
Extended source G aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr4 |
atlasSource |
ATLASv20180209 |
Extended source G aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr4 |
vphasSource |
VPHASDR3 |
Extended source G aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr4 |
vphasSource |
VPHASv20160112 |
Extended source G aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr4 |
vphasSource |
VPHASv20170222 |
Extended source G aperture mag (2.8 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr6 |
atlasSource |
ATLASDR1 |
Extended source G aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMagNoAperCorr6 |
atlasSource |
ATLASDR2 |
Extended source G aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMagNoAperCorr6 |
atlasSource |
ATLASDR3 |
Extended source G aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr6 |
atlasSource |
ATLASDR4 |
Extended source G aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr6 |
atlasSource |
ATLASDR5 |
Extended source G aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr6 |
atlasSource |
ATLASv20131127 |
Extended source G aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gAperMagNoAperCorr6 |
atlasSource |
ATLASv20160425 |
Extended source G aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr6 |
atlasSource |
ATLASv20180209 |
Extended source G aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr6 |
vphasSource |
VPHASDR3 |
Extended source G aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr6 |
vphasSource |
VPHASv20160112 |
Extended source G aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gAperMagNoAperCorr6 |
vphasSource |
VPHASv20170222 |
Extended source G aperture mag (5.7 arcsec aperture diameter) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gauSig |
atlasDetection |
ATLASDR1 |
RMS of axes of ellipse fit {catalogue TType keyword: Gaussian_sigma} |
real |
4 |
pixels |
|
src.morph.param |
These are derived from the three general intensity-weighted second moments. The equivalence between them and a generalised elliptical Gaussian Distribution is used to derive Gaussian sigma = (σa²+σb²)½ |
gauSig |
atlasDetection |
ATLASDR3 |
RMS of axes of ellipse fit {catalogue TType keyword: Gaussian_sigma} |
real |
4 |
pixels |
|
src.morph.param |
These are derived from the three general intensity-weighted second moments. The equivalence between them and a generalised elliptical Gaussian Distribution is used to derive Gaussian sigma = (σa²+σb²)½ |
gauSig |
atlasDetection |
ATLASDR4 |
RMS of axes of ellipse fit {catalogue TType keyword: Gaussian_sigma} |
real |
4 |
pixels |
|
src.morph.param |
These are derived from the three general intensity-weighted second moments. The equivalence between them and a generalised elliptical Gaussian Distribution is used to derive Gaussian sigma = (σa²+σb²)½ |
gauSig |
atlasDetection |
ATLASDR5 |
RMS of axes of ellipse fit {catalogue TType keyword: Gaussian_sigma} |
real |
4 |
pixels |
|
src.morph.param |
These are derived from the three general intensity-weighted second moments. The equivalence between them and a generalised elliptical Gaussian Distribution is used to derive Gaussian sigma = (σa²+σb²)½ |
gauSig |
atlasDetection |
ATLASv20131127 |
RMS of axes of ellipse fit {catalogue TType keyword: Gaussian_sigma} |
real |
4 |
pixels |
|
src.morph.param |
These are derived from the three general intensity-weighted second moments. The equivalence between them and a generalised elliptical Gaussian Distribution is used to derive Gaussian sigma = (σa²+σb²)½ |
gauSig |
atlasDetection |
ATLASv20160425 |
RMS of axes of ellipse fit {catalogue TType keyword: Gaussian_sigma} |
real |
4 |
pixels |
|
src.morph.param |
These are derived from the three general intensity-weighted second moments. The equivalence between them and a generalised elliptical Gaussian Distribution is used to derive Gaussian sigma = (σa²+σb²)½ |
gauSig |
atlasDetection |
ATLASv20180209 |
RMS of axes of ellipse fit {catalogue TType keyword: Gaussian_sigma} |
real |
4 |
pixels |
|
src.morph.param |
These are derived from the three general intensity-weighted second moments. The equivalence between them and a generalised elliptical Gaussian Distribution is used to derive Gaussian sigma = (σa²+σb²)½ |
gauSig |
atlasDetection, atlasDetectionUncorr |
ATLASDR2 |
RMS of axes of ellipse fit {catalogue TType keyword: Gaussian_sigma} |
real |
4 |
pixels |
|
src.morph.param |
These are derived from the three general intensity-weighted second moments. The equivalence between them and a generalised elliptical Gaussian Distribution is used to derive Gaussian sigma = (σa²+σb²)½ |
gauSig |
vphasDetection |
VPHASv20160112 |
RMS of axes of ellipse fit {catalogue TType keyword: Gaussian_sigma} |
real |
4 |
pixels |
|
src.morph.param |
These are derived from the three general intensity-weighted second moments. The equivalence between them and a generalised elliptical Gaussian Distribution is used to derive Gaussian sigma = (σa²+σb²)½ |
gauSig |
vphasDetection |
VPHASv20170222 |
RMS of axes of ellipse fit {catalogue TType keyword: Gaussian_sigma} |
real |
4 |
pixels |
|
src.morph.param |
These are derived from the three general intensity-weighted second moments. The equivalence between them and a generalised elliptical Gaussian Distribution is used to derive Gaussian sigma = (σa²+σb²)½ |
gauSig |
vphasDetection, vphasDetectionUncorr |
VPHASDR3 |
RMS of axes of ellipse fit {catalogue TType keyword: Gaussian_sigma} |
real |
4 |
pixels |
|
src.morph.param |
These are derived from the three general intensity-weighted second moments. The equivalence between them and a generalised elliptical Gaussian Distribution is used to derive Gaussian sigma = (σa²+σb²)½ |
Gauss_frac_1 |
ravedr5Source |
RAVE |
Property of multi-Gaussian distance modulus fit, see Section 9, eq. 5 |
real |
4 |
|
|
stat.fit.param |
Gauss_frac_2 |
ravedr5Source |
RAVE |
Property of multi-Gaussian distance modulus fit, see Section 9, eq. 5 |
real |
4 |
|
|
stat.fit.param |
Gauss_frac_3 |
ravedr5Source |
RAVE |
Property of multi-Gaussian distance modulus fit, see Section 9, eq. 5 |
real |
4 |
|
|
stat.fit.param |
Gauss_mean_1 |
ravedr5Source |
RAVE |
Property of multi-Gaussian distance modulus fit, see Section 9, eq. 5 |
real |
4 |
|
|
stat.fit.param |
Gauss_mean_2 |
ravedr5Source |
RAVE |
Property of multi-Gaussian distance modulus fit, see Section 9, eq. 5 |
real |
4 |
|
|
stat.fit.param |
Gauss_mean_3 |
ravedr5Source |
RAVE |
Property of multi-Gaussian distance modulus fit, see Section 9, eq. 5 |
real |
4 |
|
|
stat.fit.param |
Gauss_sigma_1 |
ravedr5Source |
RAVE |
Property of multi-Gaussian distance modulus fit, see Section 9, eq. 5 |
real |
4 |
|
|
stat.fit.param |
Gauss_sigma_2 |
ravedr5Source |
RAVE |
Property of multi-Gaussian distance modulus fit, see Section 9, eq. 5 |
real |
4 |
|
|
stat.fit.param |
Gauss_sigma_3 |
ravedr5Source |
RAVE |
Property of multi-Gaussian distance modulus fit, see Section 9, eq. 5 |
real |
4 |
|
|
stat.fit.param |
gAverageConf |
atlasSource |
ATLASDR1 |
average confidence in 2 arcsec diameter default aperture (aper3) G |
real |
4 |
|
-99999999 |
meta.code |
gAverageConf |
atlasSource |
ATLASDR2 |
average confidence in 2 arcsec diameter default aperture (aper3) G |
real |
4 |
|
-99999999 |
meta.code |
gAverageConf |
atlasSource |
ATLASDR3 |
average confidence in 2 arcsec diameter default aperture (aper3) G |
real |
4 |
|
-99999999 |
stat.likelihood;em.opt.B |
gAverageConf |
atlasSource |
ATLASDR4 |
average confidence in 2 arcsec diameter default aperture (aper3) G |
real |
4 |
|
-99999999 |
stat.likelihood;em.opt.B |
gAverageConf |
atlasSource |
ATLASDR5 |
average confidence in 2 arcsec diameter default aperture (aper3) G |
real |
4 |
|
-99999999 |
stat.likelihood;em.opt.B |
gAverageConf |
atlasSource |
ATLASv20131127 |
average confidence in 2 arcsec diameter default aperture (aper3) G |
real |
4 |
|
-99999999 |
meta.code |
gAverageConf |
atlasSource |
ATLASv20160425 |
average confidence in 2 arcsec diameter default aperture (aper3) G |
real |
4 |
|
-99999999 |
stat.likelihood;em.opt.B |
gAverageConf |
atlasSource |
ATLASv20180209 |
average confidence in 2 arcsec diameter default aperture (aper3) G |
real |
4 |
|
-99999999 |
stat.likelihood;em.opt.B |
gAverageConf |
vphasSource |
VPHASDR3 |
average confidence in 2 arcsec diameter default aperture (aper3) G |
real |
4 |
|
-99999999 |
stat.likelihood;em.opt.B |
gAverageConf |
vphasSource |
VPHASv20160112 |
average confidence in 2 arcsec diameter default aperture (aper3) G |
real |
4 |
|
-99999999 |
stat.likelihood;em.opt.B |
gAverageConf |
vphasSource |
VPHASv20170222 |
average confidence in 2 arcsec diameter default aperture (aper3) G |
real |
4 |
|
-99999999 |
stat.likelihood;em.opt.B |
gClass |
atlasSource |
ATLASDR1 |
discrete image classification flag in G |
smallint |
2 |
|
-9999 |
src.class |
gClass |
atlasSource |
ATLASDR2 |
discrete image classification flag in G |
smallint |
2 |
|
-9999 |
src.class |
gClass |
atlasSource |
ATLASDR3 |
discrete image classification flag in G |
smallint |
2 |
|
-9999 |
src.class;em.opt.B |
gClass |
atlasSource |
ATLASDR4 |
discrete image classification flag in G |
smallint |
2 |
|
-9999 |
src.class;em.opt.B |
gClass |
atlasSource |
ATLASDR5 |
discrete image classification flag in G |
smallint |
2 |
|
-9999 |
src.class;em.opt.B |
gClass |
atlasSource |
ATLASv20131127 |
discrete image classification flag in G |
smallint |
2 |
|
-9999 |
src.class |
gClass |
atlasSource |
ATLASv20160425 |
discrete image classification flag in G |
smallint |
2 |
|
-9999 |
src.class;em.opt.B |
gClass |
atlasSource |
ATLASv20180209 |
discrete image classification flag in G |
smallint |
2 |
|
-9999 |
src.class;em.opt.B |
gClass |
vphasSource |
VPHASDR3 |
discrete image classification flag in G |
smallint |
2 |
|
-9999 |
src.class;em.opt.B |
gClass |
vphasSource |
VPHASv20160112 |
discrete image classification flag in G |
smallint |
2 |
|
-9999 |
src.class;em.opt.B |
gClass |
vphasSource |
VPHASv20170222 |
discrete image classification flag in G |
smallint |
2 |
|
-9999 |
src.class;em.opt.B |
gClassStat |
atlasSource |
ATLASDR1 |
N(0,1) stellarness-of-profile statistic in G |
real |
4 |
|
-0.9999995e9 |
stat |
gClassStat |
atlasSource |
ATLASDR2 |
N(0,1) stellarness-of-profile statistic in G |
real |
4 |
|
-0.9999995e9 |
stat |
gClassStat |
atlasSource |
ATLASDR3 |
N(0,1) stellarness-of-profile statistic in G |
real |
4 |
|
-0.9999995e9 |
stat;em.opt.B |
gClassStat |
atlasSource |
ATLASDR4 |
N(0,1) stellarness-of-profile statistic in G |
real |
4 |
|
-0.9999995e9 |
stat;em.opt.B |
gClassStat |
atlasSource |
ATLASDR5 |
N(0,1) stellarness-of-profile statistic in G |
real |
4 |
|
-0.9999995e9 |
stat;em.opt.B |
gClassStat |
atlasSource |
ATLASv20131127 |
N(0,1) stellarness-of-profile statistic in G |
real |
4 |
|
-0.9999995e9 |
stat |
gClassStat |
atlasSource |
ATLASv20160425 |
N(0,1) stellarness-of-profile statistic in G |
real |
4 |
|
-0.9999995e9 |
stat;em.opt.B |
gClassStat |
atlasSource |
ATLASv20180209 |
N(0,1) stellarness-of-profile statistic in G |
real |
4 |
|
-0.9999995e9 |
stat;em.opt.B |
gClassStat |
vphasSource |
VPHASDR3 |
N(0,1) stellarness-of-profile statistic in G |
real |
4 |
|
-0.9999995e9 |
stat;em.opt.B |
gClassStat |
vphasSource |
VPHASv20160112 |
N(0,1) stellarness-of-profile statistic in G |
real |
4 |
|
-0.9999995e9 |
stat;em.opt.B |
gClassStat |
vphasSource |
VPHASv20170222 |
N(0,1) stellarness-of-profile statistic in G |
real |
4 |
|
-0.9999995e9 |
stat;em.opt.B |
gcnf |
twomass_sixx2_psc, twomass_sixx2_xsc |
TWOMASS |
Group confusion flag 0=not confused or single apparation, 1=confused |
smallint |
2 |
|
|
|
gcntr |
twomass_sixx2_psc, twomass_sixx2_xsc |
TWOMASS |
A unique identifier for the merged group of apparitions of this source |
int |
4 |
|
|
|
gEll |
atlasSource |
ATLASDR1 |
1-b/a, where a/b=semi-major/minor axes in G |
real |
4 |
|
-0.9999995e9 |
src.ellipticity |
gEll |
atlasSource |
ATLASDR2 |
1-b/a, where a/b=semi-major/minor axes in G |
real |
4 |
|
-0.9999995e9 |
src.ellipticity |
gEll |
atlasSource |
ATLASDR3 |
1-b/a, where a/b=semi-major/minor axes in G |
real |
4 |
|
-0.9999995e9 |
src.ellipticity;em.opt.B |
gEll |
atlasSource |
ATLASDR4 |
1-b/a, where a/b=semi-major/minor axes in G |
real |
4 |
|
-0.9999995e9 |
src.ellipticity;em.opt.B |
gEll |
atlasSource |
ATLASDR5 |
1-b/a, where a/b=semi-major/minor axes in G |
real |
4 |
|
-0.9999995e9 |
src.ellipticity;em.opt.B |
gEll |
atlasSource |
ATLASv20131127 |
1-b/a, where a/b=semi-major/minor axes in G |
real |
4 |
|
-0.9999995e9 |
src.ellipticity |
gEll |
atlasSource |
ATLASv20160425 |
1-b/a, where a/b=semi-major/minor axes in G |
real |
4 |
|
-0.9999995e9 |
src.ellipticity;em.opt.B |
gEll |
atlasSource |
ATLASv20180209 |
1-b/a, where a/b=semi-major/minor axes in G |
real |
4 |
|
-0.9999995e9 |
src.ellipticity;em.opt.B |
gEll |
vphasSource |
VPHASDR3 |
1-b/a, where a/b=semi-major/minor axes in G |
real |
4 |
|
-0.9999995e9 |
src.ellipticity;em.opt.B |
gEll |
vphasSource |
VPHASv20160112 |
1-b/a, where a/b=semi-major/minor axes in G |
real |
4 |
|
-0.9999995e9 |
src.ellipticity;em.opt.B |
gEll |
vphasSource |
VPHASv20170222 |
1-b/a, where a/b=semi-major/minor axes in G |
real |
4 |
|
-0.9999995e9 |
src.ellipticity;em.opt.B |
geNum |
atlasMergeLog |
ATLASDR1 |
the extension number of this G frame |
tinyint |
1 |
|
|
meta.number |
geNum |
atlasMergeLog |
ATLASDR2 |
the extension number of this G frame |
tinyint |
1 |
|
|
meta.number |
geNum |
atlasMergeLog |
ATLASDR3 |
the extension number of this G frame |
tinyint |
1 |
|
|
meta.number;em.opt.B |
geNum |
atlasMergeLog |
ATLASDR4 |
the extension number of this G frame |
tinyint |
1 |
|
|
meta.number;em.opt.B |
geNum |
atlasMergeLog |
ATLASDR5 |
the extension number of this G frame |
tinyint |
1 |
|
|
meta.id;em.opt.B |
geNum |
atlasMergeLog |
ATLASv20131127 |
the extension number of this G frame |
tinyint |
1 |
|
|
meta.number |
geNum |
atlasMergeLog |
ATLASv20160425 |
the extension number of this G frame |
tinyint |
1 |
|
|
meta.number;em.opt.B |
geNum |
atlasMergeLog |
ATLASv20180209 |
the extension number of this G frame |
tinyint |
1 |
|
|
meta.number;em.opt.B |
geNum |
vphasMergeLog |
VPHASDR3 |
the extension number of this G frame |
tinyint |
1 |
|
|
meta.number;em.opt.B |
geNum |
vphasMergeLog |
VPHASv20160112 |
the extension number of this G frame |
tinyint |
1 |
|
|
meta.number;em.opt.B |
geNum |
vphasMergeLog |
VPHASv20170222 |
the extension number of this G frame |
tinyint |
1 |
|
|
meta.number;em.opt.B |
gErrBits |
atlasSource |
ATLASDR1 |
processing warning/error bitwise flags in G |
int |
4 |
|
-99999999 |
meta.code |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
gErrBits |
atlasSource |
ATLASDR2 |
processing warning/error bitwise flags in G |
int |
4 |
|
-99999999 |
meta.code |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
gErrBits |
atlasSource |
ATLASDR3 |
processing warning/error bitwise flags in G |
int |
4 |
|
-99999999 |
meta.code;em.opt.B |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
gErrBits |
atlasSource |
ATLASDR4 |
processing warning/error bitwise flags in G |
int |
4 |
|
-99999999 |
meta.code;em.opt.B |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
gErrBits |
atlasSource |
ATLASDR5 |
processing warning/error bitwise flags in G |
int |
4 |
|
-99999999 |
meta.code;em.opt.B |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
gErrBits |
atlasSource |
ATLASv20131127 |
processing warning/error bitwise flags in G |
int |
4 |
|
-99999999 |
meta.code |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
gErrBits |
atlasSource |
ATLASv20160425 |
processing warning/error bitwise flags in G |
int |
4 |
|
-99999999 |
meta.code;em.opt.B |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
gErrBits |
atlasSource |
ATLASv20180209 |
processing warning/error bitwise flags in G |
int |
4 |
|
-99999999 |
meta.code;em.opt.B |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
gErrBits |
vphasSource |
VPHASDR3 |
processing warning/error bitwise flags in G |
int |
4 |
|
-99999999 |
meta.code;em.opt.B |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
gErrBits |
vphasSource |
VPHASv20160112 |
processing warning/error bitwise flags in G |
int |
4 |
|
-99999999 |
meta.code;em.opt.B |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
gErrBits |
vphasSource |
VPHASv20170222 |
processing warning/error bitwise flags in G |
int |
4 |
|
-99999999 |
meta.code;em.opt.B |
Apparently not actually an error bit flag, but a count of the number of zero confidence pixels in the default (2 arcsec diameter) aperture. |
gEta |
atlasSource |
ATLASDR1 |
Offset of G detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff |
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. |
gEta |
atlasSource |
ATLASDR2 |
Offset of G detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff |
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. |
gEta |
atlasSource |
ATLASDR3 |
Offset of G detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff;em.opt.B |
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. |
gEta |
atlasSource |
ATLASDR4 |
Offset of G detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff;em.opt.B |
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. |
gEta |
atlasSource |
ATLASDR5 |
Offset of G detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff;em.opt.B |
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. |
gEta |
atlasSource |
ATLASv20131127 |
Offset of G detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff |
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. |
gEta |
atlasSource |
ATLASv20160425 |
Offset of G detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff;em.opt.B |
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. |
gEta |
atlasSource |
ATLASv20180209 |
Offset of G detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff;em.opt.B |
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. |
gEta |
vphasSource |
VPHASDR3 |
Offset of G detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff;em.opt.B |
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. |
gEta |
vphasSource |
VPHASv20160112 |
Offset of G detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff;em.opt.B |
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. |
gEta |
vphasSource |
VPHASv20170222 |
Offset of G detection from master position (+north/-south) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.dec;arith.diff;em.opt.B |
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. |
gGausig |
atlasSource |
ATLASDR1 |
RMS of axes of ellipse fit in G |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param |
gGausig |
atlasSource |
ATLASDR2 |
RMS of axes of ellipse fit in G |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param |
gGausig |
atlasSource |
ATLASDR3 |
RMS of axes of ellipse fit in G |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param;em.opt.B |
gGausig |
atlasSource |
ATLASDR4 |
RMS of axes of ellipse fit in G |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param;em.opt.B |
gGausig |
atlasSource |
ATLASDR5 |
RMS of axes of ellipse fit in G |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param;em.opt.B |
gGausig |
atlasSource |
ATLASv20131127 |
RMS of axes of ellipse fit in G |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param |
gGausig |
atlasSource |
ATLASv20160425 |
RMS of axes of ellipse fit in G |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param;em.opt.B |
gGausig |
atlasSource |
ATLASv20180209 |
RMS of axes of ellipse fit in G |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param;em.opt.B |
gGausig |
vphasSource |
VPHASDR3 |
RMS of axes of ellipse fit in G |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param;em.opt.B |
gGausig |
vphasSource |
VPHASv20160112 |
RMS of axes of ellipse fit in G |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param;em.opt.B |
gGausig |
vphasSource |
VPHASv20170222 |
RMS of axes of ellipse fit in G |
real |
4 |
pixels |
-0.9999995e9 |
src.morph.param;em.opt.B |
gHlCorSMjRadAs |
atlasSource |
ATLASDR1 |
Seeing corrected half-light, semi-major axis in G band |
real |
4 |
arcsec |
-0.9999995e9 |
phys.angSize;src |
gHlCorSMjRadAs |
atlasSource |
ATLASDR2 |
Seeing corrected half-light, semi-major axis in G band |
real |
4 |
arcsec |
-0.9999995e9 |
phys.angSize;src |
gHlCorSMjRadAs |
atlasSource |
ATLASDR3 |
Seeing corrected half-light, semi-major axis in G band |
real |
4 |
arcsec |
-0.9999995e9 |
phys.angSize;em.opt.B |
gHlCorSMjRadAs |
atlasSource |
ATLASDR4 |
Seeing corrected half-light, semi-major axis in G band |
real |
4 |
arcsec |
-0.9999995e9 |
phys.angSize;em.opt.B |
gHlCorSMjRadAs |
atlasSource |
ATLASDR5 |
Seeing corrected half-light, semi-major axis in G band |
real |
4 |
arcsec |
-0.9999995e9 |
phys.angSize;em.opt.B |
gHlCorSMjRadAs |
atlasSource |
ATLASv20131127 |
Seeing corrected half-light, semi-major axis in G band |
real |
4 |
arcsec |
-0.9999995e9 |
phys.angSize;src |
gHlCorSMjRadAs |
atlasSource |
ATLASv20160425 |
Seeing corrected half-light, semi-major axis in G band |
real |
4 |
arcsec |
-0.9999995e9 |
phys.angSize;em.opt.B |
gHlCorSMjRadAs |
atlasSource |
ATLASv20180209 |
Seeing corrected half-light, semi-major axis in G band |
real |
4 |
arcsec |
-0.9999995e9 |
phys.angSize;em.opt.B |
gKronMag |
atlasSource |
ATLASDR4 |
Extended source G mag (Kron) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gKronMag |
atlasSource |
ATLASDR5 |
Extended source G mag (Kron) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gKronMag |
atlasSource |
ATLASv20180209 |
Extended source G mag (Kron) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gKronMagErr |
atlasSource |
ATLASDR4 |
Error in extended source G mag (Kron) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gKronMagErr |
atlasSource |
ATLASDR5 |
Error in extended source G mag (Kron) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gKronMagErr |
atlasSource |
ATLASv20180209 |
Error in extended source G mag (Kron) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
Glat |
ravedr5Source |
RAVE |
Latitude (J2000 GCS) |
float |
8 |
deg |
|
pos.galactic.lat |
glat |
allwise_sc |
WISE |
Galactic latitude computed from the non-moving source fit equatorial position. CAUTION: This coordinate should not be used as an astrometric reference. |
float |
8 |
deg |
|
|
glat |
catwise_2020, catwise_prelim |
WISE |
galactic latitude |
float |
8 |
deg |
|
|
glat |
twomass_psc |
TWOMASS |
Galactic latitude rounded to 0.001 deg. |
real |
4 |
degrees |
|
pos.galactic.lat |
glat |
twomass_scn |
TWOMASS |
Galactic latitude of scan center, as computed from ra and dec above. |
real |
4 |
degrees |
|
pos.galactic.lat |
glat |
twomass_sixx2_scn |
TWOMASS |
galactic latitude (decimal deg) of scan center |
float |
8 |
deg |
|
|
glat |
twomass_xsc |
TWOMASS |
Galactic latitude (decimal deg) based on peak pixel. |
real |
4 |
degrees |
|
pos.galactic.lat |
glat |
wise_allskysc |
WISE |
Galactic latitude. CAUTION: This coordinate should not be used as an astrometric reference. |
float |
8 |
degrees |
|
|
glat |
wise_prelimsc |
WISE |
Galactic latitude. CAUTION: This coordinate should not be used as an astrometric reference |
float |
8 |
degrees |
|
|
Glon |
ravedr5Source |
RAVE |
Longitude (J2000 GCS) |
float |
8 |
deg |
|
pos.galactic.lon |
glon |
allwise_sc |
WISE |
Galactic longitude, computed from the non-moving source fit equatorial position. CAUTION: This coordinate should not be used as an astrometric reference. |
float |
8 |
deg |
|
|
glon |
catwise_2020, catwise_prelim |
WISE |
galactic longitude |
float |
8 |
deg |
|
|
glon |
twomass_psc |
TWOMASS |
Galactic longitude rounded to 0.001 deg. |
real |
4 |
degrees |
|
pos.galactic.lon |
glon |
twomass_scn |
TWOMASS |
Galactic longitude of scan center, as computed from ra and dec above. |
real |
4 |
degrees |
|
pos.galactic.lon |
glon |
twomass_sixx2_scn |
TWOMASS |
galactic longitude (decimal deg) of scan center |
float |
8 |
deg |
|
|
glon |
twomass_xsc |
TWOMASS |
Galactic longitude (decimal deg) based on peak pixel. |
real |
4 |
degrees |
|
pos.galactic.lon |
glon |
wise_allskysc |
WISE |
Galactic longitude. CAUTION: This coordinate should not be used as an astrometric reference. |
float |
8 |
degrees |
|
|
glon |
wise_prelimsc |
WISE |
Galactic longitude. CAUTION: This coordinate should not be used as an astrometric reference |
float |
8 |
degrees |
|
|
gmfID |
atlasMergeLog |
ATLASDR1 |
the UID of the relevant G multiframe |
bigint |
8 |
|
|
obs.field |
gmfID |
atlasMergeLog |
ATLASDR2 |
the UID of the relevant G multiframe |
bigint |
8 |
|
|
obs.field |
gmfID |
atlasMergeLog |
ATLASDR3 |
the UID of the relevant G multiframe |
bigint |
8 |
|
|
meta.id;obs.field;em.opt.B |
gmfID |
atlasMergeLog |
ATLASDR4 |
the UID of the relevant G multiframe |
bigint |
8 |
|
|
meta.id;obs.field;em.opt.B |
gmfID |
atlasMergeLog |
ATLASDR5 |
the UID of the relevant G multiframe |
bigint |
8 |
|
|
meta.id;obs.field;em.opt.B |
gmfID |
atlasMergeLog |
ATLASv20131127 |
the UID of the relevant G multiframe |
bigint |
8 |
|
|
obs.field |
gmfID |
atlasMergeLog |
ATLASv20160425 |
the UID of the relevant G multiframe |
bigint |
8 |
|
|
meta.id;obs.field;em.opt.B |
gmfID |
atlasMergeLog |
ATLASv20180209 |
the UID of the relevant G multiframe |
bigint |
8 |
|
|
meta.id;obs.field;em.opt.B |
gmfID |
vphasMergeLog |
VPHASDR3 |
the UID of the relevant G multiframe |
bigint |
8 |
|
|
meta.id;obs.field;em.opt.B |
gmfID |
vphasMergeLog |
VPHASv20160112 |
the UID of the relevant G multiframe |
bigint |
8 |
|
|
meta.id;obs.field;em.opt.B |
gmfID |
vphasMergeLog |
VPHASv20170222 |
the UID of the relevant G multiframe |
bigint |
8 |
|
|
meta.id;obs.field;em.opt.B |
gMjd |
atlasSource |
ATLASDR3 |
The mean Modified Julian Day of each detection |
float |
8 |
day |
-0.9999995e9 |
time.epoch |
gMjd |
atlasSource |
ATLASDR4 |
The mean Modified Julian Day of each detection |
float |
8 |
day |
-0.9999995e9 |
time.epoch;em.opt.B |
gMjd |
atlasSource |
ATLASDR5 |
The mean Modified Julian Day of each detection |
float |
8 |
day |
-0.9999995e9 |
time.epoch;em.opt.B |
gMjd |
atlasSource |
ATLASv20160425 |
The mean Modified Julian Day of each detection |
float |
8 |
day |
-0.9999995e9 |
time.epoch |
gMjd |
atlasSource |
ATLASv20180209 |
The mean Modified Julian Day of each detection |
float |
8 |
day |
-0.9999995e9 |
time.epoch;em.opt.B |
gMjd |
vphasSource |
VPHASDR3 |
The mean Modified Julian Day of each detection |
float |
8 |
day |
-0.9999995e9 |
time.epoch;em.opt.B |
gMjd |
vphasSource |
VPHASv20160112 |
The mean Modified Julian Day of each detection |
float |
8 |
day |
-0.9999995e9 |
time.epoch |
gMjd |
vphasSource |
VPHASv20170222 |
The mean Modified Julian Day of each detection |
float |
8 |
day |
-0.9999995e9 |
time.epoch |
gmr_1Ext |
vphasSource |
VPHASDR3 |
Extended source colour G-R_1 (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_1Ext |
vphasSource |
VPHASv20160112 |
Extended source colour G-R_1 (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_1Ext |
vphasSource |
VPHASv20170222 |
Extended source colour G-R_1 (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_1ExtErr |
vphasSource |
VPHASDR3 |
Error on extended source colour G-R_1 |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_1ExtErr |
vphasSource |
VPHASv20160112 |
Error on extended source colour G-R_1 |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_1ExtErr |
vphasSource |
VPHASv20170222 |
Error on extended source colour G-R_1 |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_1Pnt |
vphasSource |
VPHASDR3 |
Point source colour G-R_1 (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_1Pnt |
vphasSource |
VPHASv20160112 |
Point source colour G-R_1 (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_1Pnt |
vphasSource |
VPHASv20170222 |
Point source colour G-R_1 (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_1PntErr |
vphasSource |
VPHASDR3 |
Error on point source colour G-R_1 |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_1PntErr |
vphasSource |
VPHASv20160112 |
Error on point source colour G-R_1 |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_1PntErr |
vphasSource |
VPHASv20170222 |
Error on point source colour G-R_1 |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_2Ext |
vphasSource |
VPHASDR3 |
Extended source colour G-R_2 (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_2Ext |
vphasSource |
VPHASv20160112 |
Extended source colour G-R_2 (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_2Ext |
vphasSource |
VPHASv20170222 |
Extended source colour G-R_2 (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_2ExtErr |
vphasSource |
VPHASDR3 |
Error on extended source colour G-R_2 |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_2ExtErr |
vphasSource |
VPHASv20160112 |
Error on extended source colour G-R_2 |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_2ExtErr |
vphasSource |
VPHASv20170222 |
Error on extended source colour G-R_2 |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_2Pnt |
vphasSource |
VPHASDR3 |
Point source colour G-R_2 (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_2Pnt |
vphasSource |
VPHASv20160112 |
Point source colour G-R_2 (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_2Pnt |
vphasSource |
VPHASv20170222 |
Point source colour G-R_2 (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_2PntErr |
vphasSource |
VPHASDR3 |
Error on point source colour G-R_2 |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_2PntErr |
vphasSource |
VPHASv20160112 |
Error on point source colour G-R_2 |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmr_2PntErr |
vphasSource |
VPHASv20170222 |
Error on point source colour G-R_2 |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExt |
atlasSource |
ATLASDR1 |
Extended source colour G-R (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
PHOT_COLOR |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExt |
atlasSource |
ATLASDR2 |
Extended source colour G-R (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
PHOT_COLOR |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExt |
atlasSource |
ATLASDR3 |
Extended source colour G-R (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExt |
atlasSource |
ATLASDR4 |
Extended source colour G-R (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExt |
atlasSource |
ATLASDR5 |
Extended source colour G-R (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExt |
atlasSource |
ATLASv20131127 |
Extended source colour G-R (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
PHOT_COLOR |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExt |
atlasSource |
ATLASv20160425 |
Extended source colour G-R (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExt |
atlasSource |
ATLASv20180209 |
Extended source colour G-R (using aperMagNoAperCorr3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExtErr |
atlasSource |
ATLASDR1 |
Error on extended source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExtErr |
atlasSource |
ATLASDR2 |
Error on extended source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExtErr |
atlasSource |
ATLASDR3 |
Error on extended source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExtErr |
atlasSource |
ATLASDR4 |
Error on extended source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExtErr |
atlasSource |
ATLASDR5 |
Error on extended source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExtErr |
atlasSource |
ATLASv20131127 |
Error on extended source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExtErr |
atlasSource |
ATLASv20160425 |
Error on extended source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrExtErr |
atlasSource |
ATLASv20180209 |
Error on extended source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPnt |
atlasSource |
ATLASDR1 |
Point source colour G-R (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
PHOT_COLOR |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPnt |
atlasSource |
ATLASDR2 |
Point source colour G-R (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
PHOT_COLOR |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPnt |
atlasSource |
ATLASDR3 |
Point source colour G-R (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPnt |
atlasSource |
ATLASDR4 |
Point source colour G-R (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPnt |
atlasSource |
ATLASDR5 |
Point source colour G-R (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPnt |
atlasSource |
ATLASv20131127 |
Point source colour G-R (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
PHOT_COLOR |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPnt |
atlasSource |
ATLASv20160425 |
Point source colour G-R (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPnt |
atlasSource |
ATLASv20180209 |
Point source colour G-R (using aperMag3) |
real |
4 |
mag |
-0.9999995e9 |
phot.color;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPntErr |
atlasSource |
ATLASDR1 |
Error on point source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPntErr |
atlasSource |
ATLASDR2 |
Error on point source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPntErr |
atlasSource |
ATLASDR3 |
Error on point source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPntErr |
atlasSource |
ATLASDR4 |
Error on point source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPntErr |
atlasSource |
ATLASDR5 |
Error on point source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPntErr |
atlasSource |
ATLASv20131127 |
Error on point source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPntErr |
atlasSource |
ATLASv20160425 |
Error on point source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gmrPntErr |
atlasSource |
ATLASv20180209 |
Error on point source colour G-R |
real |
4 |
mag |
-0.9999995e9 |
stat.error;em.opt.B;em.opt.R |
Default colours from pairs of adjacent passbands within a given set (e.g. Y-J, J-H and H-K for YJHK) are recorded in the merged source table for ease of querying and speedy querying via indexing of these attributes. Presently, the point-source colours and extended source colours are computed from the aperture corrected AperMag3 fixed 2 arcsec aperture diameter measures (for consistent measurement across all passbands) and generally good signal-to-noise. At some point in the future, this may be changed such that point-source colours will be computed from the PSF-fitted measures and extended source colours computed from the 2-d Sersic model profile fits. |
gPA |
atlasSource |
ATLASDR1 |
ellipse fit celestial orientation in G |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng |
gPA |
atlasSource |
ATLASDR2 |
ellipse fit celestial orientation in G |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng |
gPA |
atlasSource |
ATLASDR3 |
ellipse fit celestial orientation in G |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng;em.opt.B |
gPA |
atlasSource |
ATLASDR4 |
ellipse fit celestial orientation in G |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng;em.opt.B |
gPA |
atlasSource |
ATLASDR5 |
ellipse fit celestial orientation in G |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng;em.opt.B |
gPA |
atlasSource |
ATLASv20131127 |
ellipse fit celestial orientation in G |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng |
gPA |
atlasSource |
ATLASv20160425 |
ellipse fit celestial orientation in G |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng;em.opt.B |
gPA |
atlasSource |
ATLASv20180209 |
ellipse fit celestial orientation in G |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng;em.opt.B |
gPA |
vphasSource |
VPHASDR3 |
ellipse fit celestial orientation in G |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng;em.opt.B |
gPA |
vphasSource |
VPHASv20160112 |
ellipse fit celestial orientation in G |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng;em.opt.B |
gPA |
vphasSource |
VPHASv20170222 |
ellipse fit celestial orientation in G |
real |
4 |
Degrees |
-0.9999995e9 |
pos.posAng;em.opt.B |
gPetroMag |
atlasSource |
ATLASDR1 |
Extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gPetroMag |
atlasSource |
ATLASDR2 |
Extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gPetroMag |
atlasSource |
ATLASDR3 |
Extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPetroMag |
atlasSource |
ATLASDR4 |
Extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPetroMag |
atlasSource |
ATLASDR5 |
Extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPetroMag |
atlasSource |
ATLASv20131127 |
Extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gPetroMag |
atlasSource |
ATLASv20160425 |
Extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPetroMag |
atlasSource |
ATLASv20180209 |
Extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPetroMag |
vphasSource |
VPHASDR3 |
Extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPetroMag |
vphasSource |
VPHASv20160112 |
Extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPetroMag |
vphasSource |
VPHASv20170222 |
Extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPetroMagErr |
atlasSource |
ATLASDR1 |
Error in extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gPetroMagErr |
atlasSource |
ATLASDR2 |
Error in extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gPetroMagErr |
atlasSource |
ATLASDR3 |
Error in extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gPetroMagErr |
atlasSource |
ATLASDR4 |
Error in extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gPetroMagErr |
atlasSource |
ATLASDR5 |
Error in extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gPetroMagErr |
atlasSource |
ATLASv20131127 |
Error in extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gPetroMagErr |
atlasSource |
ATLASv20160425 |
Error in extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gPetroMagErr |
atlasSource |
ATLASv20180209 |
Error in extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gPetroMagErr |
vphasSource |
VPHASDR3 |
Error in extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gPetroMagErr |
vphasSource |
VPHASv20160112 |
Error in extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gPetroMagErr |
vphasSource |
VPHASv20170222 |
Error in extended source G mag (Petrosian) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gpmag_APASSDR9 |
ravedr5Source |
RAVE |
g' magnitude from APASSDR9 |
real |
4 |
mag |
|
phot.mag;em.opt |
gppErrBits |
atlasSource |
ATLASDR1 |
additional WFAU post-processing error bits in G |
int |
4 |
|
0 |
meta.code |
Post-processing error quality bit flags assigned to detections in the archive curation procedure for survey data. From least to most significant byte in the 4-byte integer attribute byte 0 (bits 0 to 7) corresponds to information on generally innocuous conditions that are nonetheless potentially significant as regards the integrity of that detection; byte 1 (bits 8 to 15) corresponds to warnings; byte 2 (bits 16 to 23) corresponds to important warnings; and finally byte 3 (bits 24 to 31) corresponds to severe warnings: Byte | Bit | Detection quality issue | Threshold or bit mask | Applies to | | | | Decimal | Hexadecimal | | 0 | 4 | Deblended | 16 | 0x00000010 | All VDFS catalogues | 0 | 6 | Bad pixel(s) in default aperture | 64 | 0x00000040 | All VDFS catalogues | 0 | 7 | Low confidence in default aperture | 128 | 0x00000080 | All VDFS catalogues | 1 | 12 | Lies within detector 16 region of a tile | 4096 | 0x00001000 | All catalogues from tiles | 2 | 16 | Close to saturated | 65536 | 0x00010000 | All VDFS catalogues | 2 | 17 | Photometric calibration probably subject to systematic error | 131072 | 0x00020000 | VVV only | 2 | 22 | Lies within a dither offset of the stacked frame boundary | 4194304 | 0x00400000 | All catalogues | 2 | 23 | Lies within the underexposed strip (or "ear") of a tile | 8388608 | 0x00800000 | All catalogues from tiles | 3 | 24 | Lies within an underexposed region of a tile due to missing detector | 16777216 | 0x01000000 | All catalogues from tiles | In this way, the higher the error quality bit flag value, the more likely it is that the detection is spurious. The decimal threshold (column 4) gives the minimum value of the quality flag for a detection having the given condition (since other bits in the flag may be set also; the corresponding hexadecimal value, where each digit corresponds to 4 bits in the flag, can be easier to compute when writing SQL queries to test for a given condition). For example, to exclude all Ks band sources in the VHS having any error quality condition other than informational ones, include a predicate ... AND kppErrBits ≤ 255. See the SQL Cookbook and other online pages for further information. |
gppErrBits |
atlasSource |
ATLASDR2 |
additional WFAU post-processing error bits in G |
int |
4 |
|
0 |
meta.code |
Post-processing error quality bit flags assigned to detections in the archive curation procedure for survey data. From least to most significant byte in the 4-byte integer attribute byte 0 (bits 0 to 7) corresponds to information on generally innocuous conditions that are nonetheless potentially significant as regards the integrity of that detection; byte 1 (bits 8 to 15) corresponds to warnings; byte 2 (bits 16 to 23) corresponds to important warnings; and finally byte 3 (bits 24 to 31) corresponds to severe warnings: Byte | Bit | Detection quality issue | Threshold or bit mask | Applies to | | | | Decimal | Hexadecimal | | 0 | 4 | Deblended | 16 | 0x00000010 | All VDFS catalogues | 0 | 6 | Bad pixel(s) in default aperture | 64 | 0x00000040 | All VDFS catalogues | 0 | 7 | Low confidence in default aperture | 128 | 0x00000080 | All VDFS catalogues | 1 | 12 | Lies within detector 16 region of a tile | 4096 | 0x00001000 | All catalogues from tiles | 2 | 16 | Close to saturated | 65536 | 0x00010000 | All VDFS catalogues | 2 | 17 | Photometric calibration probably subject to systematic error | 131072 | 0x00020000 | VVV only | 2 | 22 | Lies within a dither offset of the stacked frame boundary | 4194304 | 0x00400000 | All catalogues | 2 | 23 | Lies within the underexposed strip (or "ear") of a tile | 8388608 | 0x00800000 | All catalogues from tiles | 3 | 24 | Lies within an underexposed region of a tile due to missing detector | 16777216 | 0x01000000 | All catalogues from tiles | In this way, the higher the error quality bit flag value, the more likely it is that the detection is spurious. The decimal threshold (column 4) gives the minimum value of the quality flag for a detection having the given condition (since other bits in the flag may be set also; the corresponding hexadecimal value, where each digit corresponds to 4 bits in the flag, can be easier to compute when writing SQL queries to test for a given condition). For example, to exclude all Ks band sources in the VHS having any error quality condition other than informational ones, include a predicate ... AND kppErrBits ≤ 255. See the SQL Cookbook and other online pages for further information. |
gppErrBits |
atlasSource |
ATLASDR3 |
additional WFAU post-processing error bits in G |
int |
4 |
|
0 |
meta.code;em.opt.B |
Post-processing error quality bit flags assigned to detections in the archive curation procedure for survey data. From least to most significant byte in the 4-byte integer attribute byte 0 (bits 0 to 7) corresponds to information on generally innocuous conditions that are nonetheless potentially significant as regards the integrity of that detection; byte 1 (bits 8 to 15) corresponds to warnings; byte 2 (bits 16 to 23) corresponds to important warnings; and finally byte 3 (bits 24 to 31) corresponds to severe warnings: Byte | Bit | Detection quality issue | Threshold or bit mask | Applies to | | | | Decimal | Hexadecimal | | 0 | 4 | Deblended | 16 | 0x00000010 | All VDFS catalogues | 0 | 6 | Bad pixel(s) in default aperture | 64 | 0x00000040 | All VDFS catalogues | 0 | 7 | Low confidence in default aperture | 128 | 0x00000080 | All VDFS catalogues | 1 | 12 | Lies within detector 16 region of a tile | 4096 | 0x00001000 | All catalogues from tiles | 2 | 16 | Close to saturated | 65536 | 0x00010000 | All VDFS catalogues | 2 | 17 | Photometric calibration probably subject to systematic error | 131072 | 0x00020000 | VVV only | 2 | 22 | Lies within a dither offset of the stacked frame boundary | 4194304 | 0x00400000 | All catalogues | 2 | 23 | Lies within the underexposed strip (or "ear") of a tile | 8388608 | 0x00800000 | All catalogues from tiles | 3 | 24 | Lies within an underexposed region of a tile due to missing detector | 16777216 | 0x01000000 | All catalogues from tiles | In this way, the higher the error quality bit flag value, the more likely it is that the detection is spurious. The decimal threshold (column 4) gives the minimum value of the quality flag for a detection having the given condition (since other bits in the flag may be set also; the corresponding hexadecimal value, where each digit corresponds to 4 bits in the flag, can be easier to compute when writing SQL queries to test for a given condition). For example, to exclude all Ks band sources in the VHS having any error quality condition other than informational ones, include a predicate ... AND kppErrBits ≤ 255. See the SQL Cookbook and other online pages for further information. |
gppErrBits |
atlasSource |
ATLASDR4 |
additional WFAU post-processing error bits in G |
int |
4 |
|
0 |
meta.code;em.opt.B |
Post-processing error quality bit flags assigned to detections in the archive curation procedure for survey data. From least to most significant byte in the 4-byte integer attribute byte 0 (bits 0 to 7) corresponds to information on generally innocuous conditions that are nonetheless potentially significant as regards the integrity of that detection; byte 1 (bits 8 to 15) corresponds to warnings; byte 2 (bits 16 to 23) corresponds to important warnings; and finally byte 3 (bits 24 to 31) corresponds to severe warnings: Byte | Bit | Detection quality issue | Threshold or bit mask | Applies to | | | | Decimal | Hexadecimal | | 0 | 4 | Deblended | 16 | 0x00000010 | All VDFS catalogues | 0 | 6 | Bad pixel(s) in default aperture | 64 | 0x00000040 | All VDFS catalogues | 0 | 7 | Low confidence in default aperture | 128 | 0x00000080 | All VDFS catalogues | 1 | 12 | Lies within detector 16 region of a tile | 4096 | 0x00001000 | All catalogues from tiles | 2 | 16 | Close to saturated | 65536 | 0x00010000 | All VDFS catalogues | 2 | 17 | Photometric calibration probably subject to systematic error | 131072 | 0x00020000 | VVV only | 2 | 22 | Lies within a dither offset of the stacked frame boundary | 4194304 | 0x00400000 | All catalogues | 2 | 23 | Lies within the underexposed strip (or "ear") of a tile | 8388608 | 0x00800000 | All catalogues from tiles | 3 | 24 | Lies within an underexposed region of a tile due to missing detector | 16777216 | 0x01000000 | All catalogues from tiles | In this way, the higher the error quality bit flag value, the more likely it is that the detection is spurious. The decimal threshold (column 4) gives the minimum value of the quality flag for a detection having the given condition (since other bits in the flag may be set also; the corresponding hexadecimal value, where each digit corresponds to 4 bits in the flag, can be easier to compute when writing SQL queries to test for a given condition). For example, to exclude all Ks band sources in the VHS having any error quality condition other than informational ones, include a predicate ... AND kppErrBits ≤ 255. See the SQL Cookbook and other online pages for further information. |
gppErrBits |
atlasSource |
ATLASDR5 |
additional WFAU post-processing error bits in G |
int |
4 |
|
0 |
meta.code;em.opt.B |
Post-processing error quality bit flags assigned to detections in the archive curation procedure for survey data. From least to most significant byte in the 4-byte integer attribute byte 0 (bits 0 to 7) corresponds to information on generally innocuous conditions that are nonetheless potentially significant as regards the integrity of that detection; byte 1 (bits 8 to 15) corresponds to warnings; byte 2 (bits 16 to 23) corresponds to important warnings; and finally byte 3 (bits 24 to 31) corresponds to severe warnings: Byte | Bit | Detection quality issue | Threshold or bit mask | Applies to | | | | Decimal | Hexadecimal | | 0 | 4 | Deblended | 16 | 0x00000010 | All VDFS catalogues | 0 | 6 | Bad pixel(s) in default aperture | 64 | 0x00000040 | All VDFS catalogues | 0 | 7 | Low confidence in default aperture | 128 | 0x00000080 | All VDFS catalogues | 1 | 12 | Lies within detector 16 region of a tile | 4096 | 0x00001000 | All catalogues from tiles | 2 | 16 | Close to saturated | 65536 | 0x00010000 | All VDFS catalogues | 2 | 17 | Photometric calibration probably subject to systematic error | 131072 | 0x00020000 | VVV only | 2 | 22 | Lies within a dither offset of the stacked frame boundary | 4194304 | 0x00400000 | All catalogues | 2 | 23 | Lies within the underexposed strip (or "ear") of a tile | 8388608 | 0x00800000 | All catalogues from tiles | 3 | 24 | Lies within an underexposed region of a tile due to missing detector | 16777216 | 0x01000000 | All catalogues from tiles | In this way, the higher the error quality bit flag value, the more likely it is that the detection is spurious. The decimal threshold (column 4) gives the minimum value of the quality flag for a detection having the given condition (since other bits in the flag may be set also; the corresponding hexadecimal value, where each digit corresponds to 4 bits in the flag, can be easier to compute when writing SQL queries to test for a given condition). For example, to exclude all Ks band sources in the VHS having any error quality condition other than informational ones, include a predicate ... AND kppErrBits ≤ 255. See the SQL Cookbook and other online pages for further information. |
gppErrBits |
atlasSource |
ATLASv20131127 |
additional WFAU post-processing error bits in G |
int |
4 |
|
0 |
meta.code |
Post-processing error quality bit flags assigned to detections in the archive curation procedure for survey data. From least to most significant byte in the 4-byte integer attribute byte 0 (bits 0 to 7) corresponds to information on generally innocuous conditions that are nonetheless potentially significant as regards the integrity of that detection; byte 1 (bits 8 to 15) corresponds to warnings; byte 2 (bits 16 to 23) corresponds to important warnings; and finally byte 3 (bits 24 to 31) corresponds to severe warnings: Byte | Bit | Detection quality issue | Threshold or bit mask | Applies to | | | | Decimal | Hexadecimal | | 0 | 4 | Deblended | 16 | 0x00000010 | All VDFS catalogues | 0 | 6 | Bad pixel(s) in default aperture | 64 | 0x00000040 | All VDFS catalogues | 0 | 7 | Low confidence in default aperture | 128 | 0x00000080 | All VDFS catalogues | 1 | 12 | Lies within detector 16 region of a tile | 4096 | 0x00001000 | All catalogues from tiles | 2 | 16 | Close to saturated | 65536 | 0x00010000 | All VDFS catalogues | 2 | 17 | Photometric calibration probably subject to systematic error | 131072 | 0x00020000 | VVV only | 2 | 22 | Lies within a dither offset of the stacked frame boundary | 4194304 | 0x00400000 | All catalogues | 2 | 23 | Lies within the underexposed strip (or "ear") of a tile | 8388608 | 0x00800000 | All catalogues from tiles | 3 | 24 | Lies within an underexposed region of a tile due to missing detector | 16777216 | 0x01000000 | All catalogues from tiles | In this way, the higher the error quality bit flag value, the more likely it is that the detection is spurious. The decimal threshold (column 4) gives the minimum value of the quality flag for a detection having the given condition (since other bits in the flag may be set also; the corresponding hexadecimal value, where each digit corresponds to 4 bits in the flag, can be easier to compute when writing SQL queries to test for a given condition). For example, to exclude all Ks band sources in the VHS having any error quality condition other than informational ones, include a predicate ... AND kppErrBits ≤ 255. See the SQL Cookbook and other online pages for further information. |
gppErrBits |
atlasSource |
ATLASv20160425 |
additional WFAU post-processing error bits in G |
int |
4 |
|
0 |
meta.code;em.opt.B |
Post-processing error quality bit flags assigned to detections in the archive curation procedure for survey data. From least to most significant byte in the 4-byte integer attribute byte 0 (bits 0 to 7) corresponds to information on generally innocuous conditions that are nonetheless potentially significant as regards the integrity of that detection; byte 1 (bits 8 to 15) corresponds to warnings; byte 2 (bits 16 to 23) corresponds to important warnings; and finally byte 3 (bits 24 to 31) corresponds to severe warnings: Byte | Bit | Detection quality issue | Threshold or bit mask | Applies to | | | | Decimal | Hexadecimal | | 0 | 4 | Deblended | 16 | 0x00000010 | All VDFS catalogues | 0 | 6 | Bad pixel(s) in default aperture | 64 | 0x00000040 | All VDFS catalogues | 0 | 7 | Low confidence in default aperture | 128 | 0x00000080 | All VDFS catalogues | 1 | 12 | Lies within detector 16 region of a tile | 4096 | 0x00001000 | All catalogues from tiles | 2 | 16 | Close to saturated | 65536 | 0x00010000 | All VDFS catalogues | 2 | 17 | Photometric calibration probably subject to systematic error | 131072 | 0x00020000 | VVV only | 2 | 22 | Lies within a dither offset of the stacked frame boundary | 4194304 | 0x00400000 | All catalogues | 2 | 23 | Lies within the underexposed strip (or "ear") of a tile | 8388608 | 0x00800000 | All catalogues from tiles | 3 | 24 | Lies within an underexposed region of a tile due to missing detector | 16777216 | 0x01000000 | All catalogues from tiles | In this way, the higher the error quality bit flag value, the more likely it is that the detection is spurious. The decimal threshold (column 4) gives the minimum value of the quality flag for a detection having the given condition (since other bits in the flag may be set also; the corresponding hexadecimal value, where each digit corresponds to 4 bits in the flag, can be easier to compute when writing SQL queries to test for a given condition). For example, to exclude all Ks band sources in the VHS having any error quality condition other than informational ones, include a predicate ... AND kppErrBits ≤ 255. See the SQL Cookbook and other online pages for further information. |
gppErrBits |
atlasSource |
ATLASv20180209 |
additional WFAU post-processing error bits in G |
int |
4 |
|
0 |
meta.code;em.opt.B |
Post-processing error quality bit flags assigned to detections in the archive curation procedure for survey data. From least to most significant byte in the 4-byte integer attribute byte 0 (bits 0 to 7) corresponds to information on generally innocuous conditions that are nonetheless potentially significant as regards the integrity of that detection; byte 1 (bits 8 to 15) corresponds to warnings; byte 2 (bits 16 to 23) corresponds to important warnings; and finally byte 3 (bits 24 to 31) corresponds to severe warnings: Byte | Bit | Detection quality issue | Threshold or bit mask | Applies to | | | | Decimal | Hexadecimal | | 0 | 4 | Deblended | 16 | 0x00000010 | All VDFS catalogues | 0 | 6 | Bad pixel(s) in default aperture | 64 | 0x00000040 | All VDFS catalogues | 0 | 7 | Low confidence in default aperture | 128 | 0x00000080 | All VDFS catalogues | 1 | 12 | Lies within detector 16 region of a tile | 4096 | 0x00001000 | All catalogues from tiles | 2 | 16 | Close to saturated | 65536 | 0x00010000 | All VDFS catalogues | 2 | 17 | Photometric calibration probably subject to systematic error | 131072 | 0x00020000 | VVV only | 2 | 22 | Lies within a dither offset of the stacked frame boundary | 4194304 | 0x00400000 | All catalogues | 2 | 23 | Lies within the underexposed strip (or "ear") of a tile | 8388608 | 0x00800000 | All catalogues from tiles | 3 | 24 | Lies within an underexposed region of a tile due to missing detector | 16777216 | 0x01000000 | All catalogues from tiles | In this way, the higher the error quality bit flag value, the more likely it is that the detection is spurious. The decimal threshold (column 4) gives the minimum value of the quality flag for a detection having the given condition (since other bits in the flag may be set also; the corresponding hexadecimal value, where each digit corresponds to 4 bits in the flag, can be easier to compute when writing SQL queries to test for a given condition). For example, to exclude all Ks band sources in the VHS having any error quality condition other than informational ones, include a predicate ... AND kppErrBits ≤ 255. See the SQL Cookbook and other online pages for further information. |
gppErrBits |
vphasSource |
VPHASDR3 |
additional WFAU post-processing error bits in G |
int |
4 |
|
0 |
meta.code;em.opt.B |
Post-processing error quality bit flags assigned to detections in the archive curation procedure for survey data. From least to most significant byte in the 4-byte integer attribute byte 0 (bits 0 to 7) corresponds to information on generally innocuous conditions that are nonetheless potentially significant as regards the integrity of that detection; byte 1 (bits 8 to 15) corresponds to warnings; byte 2 (bits 16 to 23) corresponds to important warnings; and finally byte 3 (bits 24 to 31) corresponds to severe warnings: Byte | Bit | Detection quality issue | Threshold or bit mask | Applies to | | | | Decimal | Hexadecimal | | 0 | 4 | Deblended | 16 | 0x00000010 | All VDFS catalogues | 0 | 6 | Bad pixel(s) in default aperture | 64 | 0x00000040 | All VDFS catalogues | 0 | 7 | Low confidence in default aperture | 128 | 0x00000080 | All VDFS catalogues | 1 | 12 | Lies within detector 16 region of a tile | 4096 | 0x00001000 | All catalogues from tiles | 2 | 16 | Close to saturated | 65536 | 0x00010000 | All VDFS catalogues | 2 | 17 | Photometric calibration probably subject to systematic error | 131072 | 0x00020000 | VVV only | 2 | 22 | Lies within a dither offset of the stacked frame boundary | 4194304 | 0x00400000 | All catalogues | 2 | 23 | Lies within the underexposed strip (or "ear") of a tile | 8388608 | 0x00800000 | All catalogues from tiles | 3 | 24 | Lies within an underexposed region of a tile due to missing detector | 16777216 | 0x01000000 | All catalogues from tiles | In this way, the higher the error quality bit flag value, the more likely it is that the detection is spurious. The decimal threshold (column 4) gives the minimum value of the quality flag for a detection having the given condition (since other bits in the flag may be set also; the corresponding hexadecimal value, where each digit corresponds to 4 bits in the flag, can be easier to compute when writing SQL queries to test for a given condition). For example, to exclude all Ks band sources in the VHS having any error quality condition other than informational ones, include a predicate ... AND kppErrBits ≤ 255. See the SQL Cookbook and other online pages for further information. |
gppErrBits |
vphasSource |
VPHASv20160112 |
additional WFAU post-processing error bits in G |
int |
4 |
|
0 |
meta.code;em.opt.B |
Post-processing error quality bit flags assigned to detections in the archive curation procedure for survey data. From least to most significant byte in the 4-byte integer attribute byte 0 (bits 0 to 7) corresponds to information on generally innocuous conditions that are nonetheless potentially significant as regards the integrity of that detection; byte 1 (bits 8 to 15) corresponds to warnings; byte 2 (bits 16 to 23) corresponds to important warnings; and finally byte 3 (bits 24 to 31) corresponds to severe warnings: Byte | Bit | Detection quality issue | Threshold or bit mask | Applies to | | | | Decimal | Hexadecimal | | 0 | 4 | Deblended | 16 | 0x00000010 | All VDFS catalogues | 0 | 6 | Bad pixel(s) in default aperture | 64 | 0x00000040 | All VDFS catalogues | 0 | 7 | Low confidence in default aperture | 128 | 0x00000080 | All VDFS catalogues | 1 | 12 | Lies within detector 16 region of a tile | 4096 | 0x00001000 | All catalogues from tiles | 2 | 16 | Close to saturated | 65536 | 0x00010000 | All VDFS catalogues | 2 | 17 | Photometric calibration probably subject to systematic error | 131072 | 0x00020000 | VVV only | 2 | 22 | Lies within a dither offset of the stacked frame boundary | 4194304 | 0x00400000 | All catalogues | 2 | 23 | Lies within the underexposed strip (or "ear") of a tile | 8388608 | 0x00800000 | All catalogues from tiles | 3 | 24 | Lies within an underexposed region of a tile due to missing detector | 16777216 | 0x01000000 | All catalogues from tiles | In this way, the higher the error quality bit flag value, the more likely it is that the detection is spurious. The decimal threshold (column 4) gives the minimum value of the quality flag for a detection having the given condition (since other bits in the flag may be set also; the corresponding hexadecimal value, where each digit corresponds to 4 bits in the flag, can be easier to compute when writing SQL queries to test for a given condition). For example, to exclude all Ks band sources in the VHS having any error quality condition other than informational ones, include a predicate ... AND kppErrBits ≤ 255. See the SQL Cookbook and other online pages for further information. |
gppErrBits |
vphasSource |
VPHASv20170222 |
additional WFAU post-processing error bits in G |
int |
4 |
|
0 |
meta.code;em.opt.B |
Post-processing error quality bit flags assigned to detections in the archive curation procedure for survey data. From least to most significant byte in the 4-byte integer attribute byte 0 (bits 0 to 7) corresponds to information on generally innocuous conditions that are nonetheless potentially significant as regards the integrity of that detection; byte 1 (bits 8 to 15) corresponds to warnings; byte 2 (bits 16 to 23) corresponds to important warnings; and finally byte 3 (bits 24 to 31) corresponds to severe warnings: Byte | Bit | Detection quality issue | Threshold or bit mask | Applies to | | | | Decimal | Hexadecimal | | 0 | 4 | Deblended | 16 | 0x00000010 | All VDFS catalogues | 0 | 6 | Bad pixel(s) in default aperture | 64 | 0x00000040 | All VDFS catalogues | 0 | 7 | Low confidence in default aperture | 128 | 0x00000080 | All VDFS catalogues | 1 | 12 | Lies within detector 16 region of a tile | 4096 | 0x00001000 | All catalogues from tiles | 2 | 16 | Close to saturated | 65536 | 0x00010000 | All VDFS catalogues | 2 | 17 | Photometric calibration probably subject to systematic error | 131072 | 0x00020000 | VVV only | 2 | 22 | Lies within a dither offset of the stacked frame boundary | 4194304 | 0x00400000 | All catalogues | 2 | 23 | Lies within the underexposed strip (or "ear") of a tile | 8388608 | 0x00800000 | All catalogues from tiles | 3 | 24 | Lies within an underexposed region of a tile due to missing detector | 16777216 | 0x01000000 | All catalogues from tiles | In this way, the higher the error quality bit flag value, the more likely it is that the detection is spurious. The decimal threshold (column 4) gives the minimum value of the quality flag for a detection having the given condition (since other bits in the flag may be set also; the corresponding hexadecimal value, where each digit corresponds to 4 bits in the flag, can be easier to compute when writing SQL queries to test for a given condition). For example, to exclude all Ks band sources in the VHS having any error quality condition other than informational ones, include a predicate ... AND kppErrBits ≤ 255. See the SQL Cookbook and other online pages for further information. |
gPsfMag |
atlasSource |
ATLASDR1 |
Point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gPsfMag |
atlasSource |
ATLASDR2 |
Point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gPsfMag |
atlasSource |
ATLASDR3 |
Point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPsfMag |
atlasSource |
ATLASv20131127 |
Point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gPsfMag |
atlasSource |
ATLASv20160425 |
Point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPsfMag |
vphasSource |
VPHASDR3 |
Point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPsfMag |
vphasSource |
VPHASv20160112 |
Point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPsfMag |
vphasSource |
VPHASv20170222 |
Point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gPsfMagErr |
atlasSource |
ATLASDR1 |
Error in point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gPsfMagErr |
atlasSource |
ATLASDR2 |
Error in point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gPsfMagErr |
atlasSource |
ATLASDR3 |
Error in point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gPsfMagErr |
atlasSource |
ATLASv20131127 |
Error in point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gPsfMagErr |
atlasSource |
ATLASv20160425 |
Error in point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gPsfMagErr |
vphasSource |
VPHASDR3 |
Error in point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gPsfMagErr |
vphasSource |
VPHASv20160112 |
Error in point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gPsfMagErr |
vphasSource |
VPHASv20170222 |
Error in point source profile-fitted G mag |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gsc2Class |
first08Jul16Source |
FIRST |
morphological classification in GSC-2 version 2.3.2 (s=stellar, g=nonstellar/galaxy) |
varchar |
1 |
|
|
|
gsc2Mag |
first08Jul16Source |
FIRST |
GSC2 F magnitude |
real |
4 |
mag |
|
|
gsc2Matches |
first08Jul16Source |
FIRST |
number of matches within a fiducial radius (10 arcsec) with GSC-2 version 2.3.2 |
int |
4 |
|
|
|
gsc2Sep |
first08Jul16Source |
FIRST |
separation of the nearest match in GSC-2 version 2.3.2 from the FIRST position |
real |
4 |
arcsec |
|
|
gSeqNum |
atlasSource |
ATLASDR1 |
the running number of the G detection |
int |
4 |
|
-99999999 |
meta.id |
gSeqNum |
atlasSource |
ATLASDR2 |
the running number of the G detection |
int |
4 |
|
-99999999 |
meta.id |
gSeqNum |
atlasSource |
ATLASDR3 |
the running number of the G detection |
int |
4 |
|
-99999999 |
meta.number;em.opt.B |
gSeqNum |
atlasSource |
ATLASDR4 |
the running number of the G detection |
int |
4 |
|
-99999999 |
meta.number;em.opt.B |
gSeqNum |
atlasSource |
ATLASDR5 |
the running number of the G detection |
int |
4 |
|
-99999999 |
meta.id;em.opt.B |
gSeqNum |
atlasSource |
ATLASv20131127 |
the running number of the G detection |
int |
4 |
|
-99999999 |
meta.id |
gSeqNum |
atlasSource |
ATLASv20160425 |
the running number of the G detection |
int |
4 |
|
-99999999 |
meta.number;em.opt.B |
gSeqNum |
atlasSource |
ATLASv20180209 |
the running number of the G detection |
int |
4 |
|
-99999999 |
meta.number;em.opt.B |
gSeqNum |
vphasSource |
VPHASDR3 |
the running number of the G detection |
int |
4 |
|
-99999999 |
meta.number;em.opt.B |
gSeqNum |
vphasSource |
VPHASv20160112 |
the running number of the G detection |
int |
4 |
|
-99999999 |
meta.number;em.opt.B |
gSeqNum |
vphasSource |
VPHASv20170222 |
the running number of the G detection |
int |
4 |
|
-99999999 |
meta.number;em.opt.B |
gSerMag2D |
atlasSource |
ATLASDR1 |
Extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gSerMag2D |
atlasSource |
ATLASDR2 |
Extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gSerMag2D |
atlasSource |
ATLASDR3 |
Extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gSerMag2D |
atlasSource |
ATLASv20131127 |
Extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag |
gSerMag2D |
atlasSource |
ATLASv20160425 |
Extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gSerMag2D |
vphasSource |
VPHASDR3 |
Extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gSerMag2D |
vphasSource |
VPHASv20160112 |
Extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gSerMag2D |
vphasSource |
VPHASv20170222 |
Extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
phot.mag;em.opt.B |
gSerMag2DErr |
atlasSource |
ATLASDR1 |
Error in extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gSerMag2DErr |
atlasSource |
ATLASDR2 |
Error in extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gSerMag2DErr |
atlasSource |
ATLASDR3 |
Error in extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gSerMag2DErr |
atlasSource |
ATLASv20131127 |
Error in extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
stat.error |
gSerMag2DErr |
atlasSource |
ATLASv20160425 |
Error in extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gSerMag2DErr |
vphasSource |
VPHASDR3 |
Error in extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gSerMag2DErr |
vphasSource |
VPHASv20160112 |
Error in extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gSerMag2DErr |
vphasSource |
VPHASv20170222 |
Error in extended source G mag (profile-fitted) |
real |
4 |
mag |
-0.9999995e9 |
stat.error;phot.mag;em.opt.B |
gXi |
atlasSource |
ATLASDR1 |
Offset of G detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff |
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. |
gXi |
atlasSource |
ATLASDR2 |
Offset of G detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff |
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. |
gXi |
atlasSource |
ATLASDR3 |
Offset of G detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff;em.opt.B |
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. |
gXi |
atlasSource |
ATLASDR4 |
Offset of G detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff;em.opt.B |
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. |
gXi |
atlasSource |
ATLASDR5 |
Offset of G detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff;em.opt.B |
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. |
gXi |
atlasSource |
ATLASv20131127 |
Offset of G detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff |
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. |
gXi |
atlasSource |
ATLASv20160425 |
Offset of G detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff;em.opt.B |
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. |
gXi |
atlasSource |
ATLASv20180209 |
Offset of G detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff;em.opt.B |
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. |
gXi |
vphasSource |
VPHASDR3 |
Offset of G detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff;em.opt.B |
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. |
gXi |
vphasSource |
VPHASv20160112 |
Offset of G detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff;em.opt.B |
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. |
gXi |
vphasSource |
VPHASv20170222 |
Offset of G detection from master position (+east/-west) |
real |
4 |
arcsec |
-0.9999995e9 |
pos.eq.ra;arith.diff;em.opt.B |
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. |