The following table contains brief descriptions of the parameters provided for each source in the 2MASS All Sky Release PSC. The table is organized according to the broad function and utility of the parameters: positional information, photometric information, and source quality information. For PSC flag parameters, the meaning of each possible flag value is given, along with some practical information on their usage.
The columns in the following table are:
Column Name | Format | Units | nulls | Description | ||
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Primary Positional Information | ||||||
ra | %10.6f | deg | no | J2000 right ascension with respect to the ICRS | ||
dec/decl | %10.6f | deg | no | J2000 declination with respect to the ICRS | ||
err_maj | %4.2f | arcsec | no | Semi-major axis length of the one sigma position uncertainty ellipse | ||
err_min | %4.2f | arcsec | no | Semi-minor axis length of the one sigma position uncertainty ellipse | ||
err_ang | %3d | deg | no | Position angle on the sky of the semi-major axis of the position uncertainty ellipse (East of North) |   | |
designation | %17s | --- | no | Sexagesimal, equatorial position-based source name in the form: hhmmssss+ddmmsss[ABC...]. The full naming convention for 2MASS All-Sky Release PSC sources has the form "2MASS Jhhmmssss+ddmmsss[ABC...]", where "2MASS" indicates that the source is from the All-Sky PSC, "J" indicates the position is J2000, and the optional trailing letters are used to distinguish sources with otherwise duplicate names. The "2MASS J" prefix is not listed explicitly in the designation column. | ||
Primary Photometric Information | ||||||
j_m | %6.3f | mag | yes | Default J-band magnitude, or if the source is not detected in the J-band, the 95% confidence upper limit derived from a 4" radius aperture measurement taken at the position of the source on the Atlas Image. The origin of the default magnitude is given by the first character of the rd_flg value (rd_flg[1]). This column is null if the source is nominally detected in the J-band, but no useful brightness estimate could be made (rd_flg[1]="9"). | ||
j_cmsig | %5.3f | mag | yes | Corrected photometric uncertainty for the default J-band magnitude. If rd_flg[1]="2", this is the measurement error from the profile-fitting procedure, corrected to be consistent with observed repeatability statistics. If rd_flg[1]="1" or "4", this is the RMS of the brightness measured in aperture photometry on the individual frames. If rd_flg="3", the uncertainty is derived from the residuals to the 1-d radial profile fit to the unsaturated wings of the bright star. If j_cmsig > 8.0, it is a flag value indicating that a meaningful uncertainty could not be determined for the source. This column is null if the default magnitude is a 95% confidence upper limit (rd_flg[1]="0" or "6") or if the source is not measurable (rd_flg[1]="9"). | ||
j_msigcom | %5.3f | mag | yes | Combined, or total photometric uncertainty for the default J-band magnitude.
The combined uncertainty is derived from the following relation: where
j_cmsig = Corrected J-band photometric uncertainty This column is null if the default magnitude is a 95% confidence upper limit (i.e. the source is not detected, or inconsistently deblended in the J-band). |
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j_snr | %10.1f | mag | yes | J-band "scan" signal-to-noise ratio. This value is given by the ratio of the J-band flux to the characteristic J-band scan noise. The scan noise is the mode of the distribution of flux uncertainties for all point source measurements in a specific 2MASS scan, and is tabulated in the Scan Information Table (NOT YET AVAILABLE). j_snr values are capped at 10000000.0. This column is null if the default magnitude is a 95% confidence upper limit (i.e. the source is not detected, or inconsistently deblended in the J-band). | ||
h_m | %6.3f | mag | yes | Default H-band magnitude, or if the source is not detected in the H-band, the 95% confidence upper limit derived from a 4" radius aperture measurement taken at the position of the source on the Atlas Image. The origin of the default magnitude is given by the second character of the rd_flg value (rd_flg[2]). This column is null if the source is nominally detected in the H-band, but no useful brightness estimate could be made (rd_flg[2]="9"). | ||
h_cmsig | %5.3f | mag | yes | Corrected photometric uncertainty for the default H-band magnitude. If rd_flg[2]="2", this is the measurement error from the profile-fitting procedure, corrected to be consistent with observed repeatability statistics. If rd_flg[2]="1" or "4", this is the RMS of the brightness measured in aperture photometry on the individual frames. If rd_flg="3", the uncertainty is derived from the residuals to the 1-d radial profile fit to the unsaturated wings of the bright star. If h_cmsig > 8.0, it is a flag value indicating that a meaningful uncertainty could not be determined for the source. This column is null if the default magnitude is a 95% confidence upper limit (rd_flg[2]="0" or "6") or if the source is not measurable (rd_flg[2]="9"). | ||
h_msigcom | %5.3f | mag | yes | Combined, or total photometric uncertainty for the default H-band magnitude.
The combined uncertainty is derived from the following relation: where
h_cmsig = Corrected H-band photometric uncertainty This column is null if the default magnitude is a 95% confidence upper limit (i.e. the source is not detected, or inconsistently deblended in the H-band). |
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h_snr | %10.1f | mag | yes | H-band "scan" signal-to-noise ratio. This value is given by the ratio of the H-band flux to the characteristic H-band scan noise. The scan noise is the mode of the distribution of flux uncertainties for all point source measurements in a specific 2MASS scan, and is tabulated in the Scan Information Table (NOT YET AVAILABLE). h_snr values are capped at 10000000.0. This column is null if the default magnitude is a 95% confidence upper limit (i.e. the source is not detected, or inconsistently deblended in the H-band). | ||
k_m | %6.3f | mag | yes | Default Ks-band magnitude, or if the source is not detected in the Ks-band, the 95% confidence upper limit derived from a 4" radius aperture measurement taken at the position of the source on the Atlas Image. The origin of the default magnitude is given by the third character of the rd_flg value (rd_flg[3]). This column is null if the source is nominally detected in the Ks-band, but no useful brightness estimate could be made (rd_flg[3]="9"). | ||
k_cmsig | %5.3f | mag | yes | Corrected photometric uncertainty for the default Ks-band magnitude. If rd_flg[3]="2", this is the measurement error from the profile-fitting procedure, corrected to be consistent with observed repeatability statistics. If rd_flg[3]="1" or "4", this is the RMS of the brightness measured in aperture photometry on the individual frames. If rd_flg="3", the uncertainty is derived from the residuals to the 1-d radial profile fit to the unsaturated wings of the bright star. If k_cmsig > 8.0, it is a flag value indicating that a meaningful uncertainty could not be determined for the source. This column is null if the default magnitude is a 95% confidence upper limit (rd_flg[3]="0" or "6") or if the source is not measurable (rd_flg[3]="9"). | ||
k_msigcom | %5.3f | mag | yes | Combined, or total photometric uncertainty for the default Ks-band magnitude.
The combined uncertainty is derived from the following relation: where
k_cmsig = Corrected Ks-band photometric uncertainty This column is null if the default magnitude is a 95% confidence upper limit (i.e. the source is not detected, or inconsistently deblended in the Ks-band). |
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k_snr | %10.1f | mag | yes | Ks-band "scan" signal-to-noise ratio. This value is given by the ratio of the Ks-band flux to the characteristic Ks-band scan noise. The scan noise is the mode of the distribution of flux uncertainties for all point source measurements in a specific 2MASS scan, and is tabulated in the Scan Information Table (NOT YET AVAILABLE). k_snr values are capped at 10000000.0. This column is null if the default magnitude is a 95% confidence upper limit (i.e. the source is not detected, or inconsistently deblended in the Ks-band). | ||
Primary Source Quality Information | ||||||
ph_qual | %3s | --- | no | Photometric quality flag. Three character flag, one character per band [JHKs], that provides a summary of the net quality of the default photometry in each band, as derived from the Read Flag (rd_flg), measurement uncertainties ([jhk]_cmsig), scan signal-to-noise ratios ([jhk]_snr), frame-detection statistics (ndet), and profile-fit reduced chi-squared values ([jhk]_psfchi). The value for ph_qual is set for a band according to the precedence of the table below. For example, a source that is tested and meets the conditions for category "X" is not tested for subsequent qualities.
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rd_flg | %3s | --- | no | Read flag. Three character flag, one character per band [JHKs],
that indicates the origin of the default magnitudes and uncertainties
in each band (j_m,h_m,k_m,
j_cmsig, h_cmsig,
k_cmsig). Rd_flg values of "1", "2" or "3"
generally indicate the best quality detections, photometry and astrometry
(although other quality flags must be considered).
Values of "0", "4", "6" and "9" in a band indicate either non-detections,
or generally poor quality photometry and positions. The definitions
of the rd_flg values are:
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bl_flg | %3s | --- | no | Blend flag. Three character flag, one character per band [JHKs],
that indicates the number of components that were fit simultaneously
when estimating the brightness of a source:
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cc_flg | %3s | --- | no | Contamination and confusion flag. Three character flag, one character
per band [JHKs], that indicates that the photometry and/or position
measurements of a source may be contaminated or biased due to proximity
to an image artifact or nearby source of equal or greater brightness.
The cc_flg in each band is
set in hierarchical order according to the following table, in the event
a source is affected by more than one artifact or condition:
Non-zero values the cc_flg in any band is an indicator that the measurements of that source may be contaminated. |
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ndet | %6s | --- | no | Frame detection statistics. A six-character flag, two characters
per band [JJHHKsKs], that indicates the number
frames on which a source was detected, N, and the number of frames on
which the source could have been measured, M. The first digit in the
pair for each band, N, gives the number of frames on which there were
>3 sigma aperture photometry detections of the source. The second digit
for each band, M, gives the number of frames on which aperture
measurements were possible. Normally, M=6, (occasionally
M=7 because the scanning step size was
slightly less than 1/6 of the frame size). M can be <6
if frames are "lost" because: a) there were masked pixels
within the source aperture due
to cosmic ray detections, noisy pixels, meteor trails, etc,
or b) there were saturated pixels within the source aperture.
Values of M < 6 are not uncommon, but do indicate
an effective loss of coverage and sensitivity for a source.
The values of N and M for a band always pertain to the aperture photometry on the 51 ms "Read_1" exposures if rd_flg="1", and to the aperture photometry on the 1.3 s "Read_2" exposures if rd_flg="2" or "4". Sources that are saturated on all of the Read_1 frames (rd_flg="3") have N=0 because no aperture photometry was possible. Sources with signal-to-noise ratios >8-9 should be detected on all available frames. Values of N < M for such sources are an indication of possible loss of measurement integrity. Values of N < M, or even N=0, are normal for fainter sources because they are too faint on individual frames to yield a >3 sigma detection. |
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prox | %5.1f | arcsec | no | Proximity. The distance between this source and its nearest neighbor in the PSC. The pts_key of the nearest source is given in the pxcntr column. The effective resolution of the 2MASS system is approximately 5". Any source with prox < 6" is potentially confused with a nearby object, and should be used with caution. | ||
pxpa | %3d | deg | yes | The position angle on the sky of the vector from the source to the nearest neighbor in the PSC, in degrees East of North. This column in null if prox=0.0, which occurs only for confused sources or from errors in the bandmerge process caused by confusion. | ||
pxcntr | %10d | --- | no | The pts_key value of the nearest source in the PSC. | ||
gal_contam | %1d | --- | no | Extended source "contamination" flag. A value of gal_contam="2"
indicates that this point source
falls within the elliptical boundary of an XSC source defined by the
semi-major axis and ellipticity of the 20 mag arcsec-2
Ks-band elliptical isophote
(r_k20fe) +10%,
for XSC sources where r_k20fe is >10''.
Sources so indicated are often foreground stars superimposed on
background galaxies, or sometimes extractions of pieces of the
galaxy or nebula.
The point source photometry for these sources is probably contaminated
by the surrounding structured extended emission.
Point sources can still be superimposed on extended sources
and remain unflagged if the XSC source shape is not well-described
by an ellipse.
This flag also denotes (gal_contam="1") PSC sources that are equivalent to sources in the XSC, but only for XSC sources with r_k20fe is >10''. Since most XSC sources have semi-major axes <10'', gal_contam does not identify all PSC sources with exact XSC counterparts. Use the ext_key to identify all PSC sources that were found to be resolved relative to a single point-spread function..
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mp_flg | %1d | --- | no | Minor Planet Flag. Indicates if this source is
associated with the predicted position of a known minor planet, comet,
planet or planetary satellite. This association does not
guarantee that the PSC source is a detection of the solar system
object.
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Additional Positional and Identification Information | ||||||
pts_key/cntr | %10d | --- | no | A unique identification number for the PSC source. This column is called pts_key in the DVD and ftp versions of the PSC and cntr in the IRSA/GATOR version. This sequential number was defined when source records from final data processing were loaded into the Point Source Working Database. Pts_key is incremented in order (or reverse order depending on the scan direction) of declination within a scan. For this reason, on average sources with close pts_key values are close to each other on the sky, except at Tile boundaries. Pts_key ordering thus provides a useful mapping of the 2MASS release on storage media. PSC sources are cross-referenced in the XSC, Known Asteroid Detection List, Known Comet Detection List, and Planet and Planetary Satellite Detection List via the value of pts_key. | ||
hemis | %1s | --- | no | Hemisphere code for the 2MASS Observatory from which this source
was observed.
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date | %10s | yyyy-mm-dd | no | The observation reference date for this source expressed in ISO standard format. This is the UT day value at sunrise for the night on which the source was observed. Because it is possible for the UT day to change during a night of observations, the actual UT date for a source measurement can differ from date by one day. Use the Julian Day value (jdate) for a more accurate determination of the observation time of the source. | ||
scan | %3d | --- | no | The nightly scan number in which the source was detected. | ||
glon | %7.3f | deg | no | Galactic longitude. Galactic coordinate for 2MASS source derived by precessing reconstructed ra and dec to B1950, and performing rotational transformation into lII, bII coordinate system. This coordinate should not be used as an astrometric reference because it has been rounded to 0.001 deg. | ||
glat | %7.3f | deg | no | Galactic latitude. Galactic coordinate for 2MASS source derived by precessing reconstructed ra and dec to B1950, and performing rotational transformation into lII, bII coordinate system. This coordinate should not be used as an astrometric reference because it has been rounded to 0.001 deg. | ||
x_scan | %6.1f | arcsec | no | Mean cross-scan focal plane position of the source in the Universal scan (U-scan) coordinate system. This is the approximate distance a source lies west or east of the focal plane centerline. Positive values of x_scan indicate that the source falls west of the centerline and negative values indicate the source is east of the centerline. The focal plane position is approximate because it is derived from the mean position of the source detected on up to seven different frames and three different bands. The U-scan coordinate system combines the pixels from the three arrays from each camera, and follows the near-great-circle path of the scan across the sky. The x_scan value is useful for identifying sources that may be caused or affected by hot pixel events. | ||
jdate | %12.4f | day | no | The Julian Date of the source measurement accurate to +30 seconds. This value is extrapolated from the start time of the Survey scan using the difference between the declinations of the source and the first row in the Tile divided by the scanning rate of the telescope (approximately 57"/sec). The scanning rate of the two 2MASS telescopes was slightly different because of the need to optimize the dithering of images on the arrays. | ||
Additional Photometric Information | ||||||
j_psfchi | %6.2f | --- | yes | Reduced chi-squared goodness-of-fit
value for the J-band profile-fit photometry
made on the 1.3 s "Read_2" exposures. Unresolved sources that
are well-fit by a single PSF should have j_psfchi~1.0.
Values >2 indicate that the source was not well-fit by a single PSF
and that the profile-fitting
measurement may not accurately capture the flux of the object.
This can occur if the source is resolved, part of a multiple star
group, or is corrupted by a cosmic ray or hot pixel event.
The j_psfchi value is useful as an indicator of photometric quality only if rd_flg[1]="2" for the source, indicating that the default J magnitude (j_m) is from a profile-fitting measurement. A non-null value for j_psfchi may be listed for sources that have rd_flg[1]="1". However, these are the goodness-of-fits made on saturated star images on the "Read_2" exposures, and do not relate to the aperture photometry magnitude reported in j_m in these cases. This field is null for rd_flg[1]="0","3","4","6" or "9". |
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h_psfchi | %6.2f | --- | yes | Reduced chi-squared goodness-of-fit
value for the H-band profile-fit photometry
made on the 1.3 s "Read_2" exposures. Unresolved sources that
are well-fit by a single PSF should have h_psfchi~1.0.
Values >2 indicate that the source was not well-fit by a single PSF
and that the profile-fitting
measurement may not accurately capture the flux of the object.
This can occur if the source is resolved, part of a multiple star
group, or is corrupted by a cosmic ray or hot pixel event.
The h_psfchi value is useful as an indicator of photometric quality only if rd_flg[2]="2" for the source, indicating that the default H magnitude (h_m) is from a profile-fitting measurement. A non-null value for h_psfchi may be listed for sources that have rd_flg[2]="1". However, these are the goodness-of-fits made on saturated star images on the "Read_2" exposures, and do not relate to the aperture photometry magnitude reported in h_m in these cases. This field is null for rd_flg[2]="0","3","4","6" or "9". |
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k_psfchi | %6.2f | --- | yes | Reduced chi-squared goodness-of-fit
value for the Ks-band profile-fit photometry
made on the 1.3 s "Read_2" exposures. Unresolved sources that
are well-fit by a single PSF should have k_psfchi~1.0.
Values >2 indicate that the source was not well-fit by a single PSF
and that the profile-fitting
measurement may not accurately capture the flux of the object.
This can occur if the source is resolved, part of a multiple star
group, or is corrupted by a cosmic ray or hot pixel event.
The k_psfchi value is useful as an indicator of photometric quality only if rd_flg[3]="2" for the source, indicating that the default J magnitude (k_m) is from a profile-fitting measurement. A non-null value for k_psfchi may be listed for sources that have rd_flg[3]="1". However, these are the goodness-of-fits made on saturated star images on the "Read_2" exposures, and do not relate to the aperture photometry magnitude reported in k_m in these cases. This field is null for rd_flg[3]="0","3","4","6" or "9". |
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j_m_stdap | %6.3f | mag | yes | J-band "standard" aperture magnitude. This is the
curve-of-growth corrected
average brightness measured in a 4" radius aperture centered
on the source position on each of the available 1.3 s "Read_2" frames.
The background
sky reference on each frame is measured in an annular region with
inner radius of 14" and outer radius of 20". Non-detections on
individual frames are included in the average so that the flux is
not statistically overestimated. The
curve-of-growth correction
adjusts to an "infinite" aperture
using a normalization value derived from a series of multi-aperture
measurements made from many stars having the same seeing FWHM
as the source that is corrected. The amplitude of the
correction is tabulated in the j_ap_cor value in the
Atlas Image Data Table (NOT YET AVAILABLE).
This column can contain a measurement even if the default magnitude is from the 51 ms "Read_1" exposures (rd_flg="1"). In this case, the value is the aperture measurement from the available non-saturated 1.3 s "Read_2" exposures. This column is null if the source is not detected in the J-band (rd_flg[1]="0"), or if it is saturated in all of the 1.3 s "Read 2" J-band exposures. |
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j_msig_stdap | %5.3f | mag | yes | Uncertainty in the J-band standard aperture magnitude.
If there was more than one 1.3 s "Read_2" frame available for
aperture photometry, this the RMS residual of the brightness measured on
the individual frames. If there was only one frame available, this
is the uncertainty derived from the single measurement using the
poisson statistics of the fluxes in the aperture and sky annulus.
This column is null if the source is not detected in the J-band (rd_flg[1]="0"), or if it is saturated in all of the 1.3 s "Read 2" J-band exposures. |
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h_m_stdap | %6.3f | mag | yes | H-band "standard" aperture magnitude. This is the
curve-of-growth corrected
average brightness measured in a 4" radius aperture centered
on the source position on each of the available 1.3 s "Read_2" frames.
The background
sky reference on each frame is measured in an annular region with
inner radius of 14" and outer radius of 20". Non-detections on
individual frames are included in the average so that the flux is
not statistically overestimated. The
curve-of-growth correction
adjusts to an "infinite" aperture
using a normalization value derived from a series of multi-aperture
measurements made from many stars having the same seeing FWHM
as the source that is corrected. The amplitude of the
correction is tabulated in the h_ap_cor value in the
Atlas Image Data Table (NOT YET AVAILABLE).
This column can contain a measurement even if the default magnitude is from the 51 ms "Read_1" exposures (rd_flg="1"). In this case, the value is the aperture measurement from the available non-saturated 1.3 s "Read_2" exposures. This column is null if the source is not detected in the H-band (rd_flg[1]="0"), or if it is saturated in all of the 1.3 s "Read 2" H-band exposures. |
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h_msig_stdap | %5.3f | mag | yes | Uncertainty in the H-band standard aperture magnitude.
If there was more than one 1.3 s "Read_2" frame available for
aperture photometry, this the RMS residual of the brightness measured on
the individual frames. If there was only one frame available, this
is the uncertainty derived from the single measurement using the
poisson statistics of the fluxes in the aperture and sky annulus.
This column is null if the source is not detected in the H-band (rd_flg[2]="0"), or if it is saturated in all of the 1.3 s "Read 2" H-band exposures. |
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k_m_stdap | %6.3f | mag | yes | Ks-band "standard" aperture magnitude. This is the
curve-of-growth corrected
average brightness measured in a 4" radius aperture centered
on the source position on each of the available 1.3 s "Read_2" frames.
The background
sky reference on each frame is measured in an annular region with
inner radius of 14" and outer radius of 20". Non-detections on
individual frames are included in the average so that the flux is
not statistically overestimated. The
curve-of-growth correction
adjusts to an "infinite" aperture
using a normalization value derived from a series of multi-aperture
measurements made from many stars having the same seeing FWHM
as the source that is corrected. The amplitude of the
correction is tabulated in the k_ap_cor value in the
Atlas Image Data Table (NOT YET AVAILABLE).
This column can contain a measurement even if the default magnitude is from the 51 ms "Read_1" exposures (rd_flg="1"). In this case, the value is the aperture measurement from the available non-saturated 1.3 s "Read_2" exposures. This column is null if the source is not detected in the Ks-band (rd_flg[1]="0"), or if it is saturated in all of the 1.3 s "Read 2" Ks-band exposures. |
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k_msig_stdap | %5.3f | mag | yes | Uncertainty in the Ks-band standard aperture magnitude.
If there was more than one 1.3 s "Read_2" frame available for
aperture photometry, this the RMS residual of the brightness measured on
the individual frames. If there was only one frame available, this
is the uncertainty derived from the single measurement using the
poisson statistics of the fluxes in the aperture and sky annulus.
This column is null if the source is not detected in the Ks-band (rd_flg[3]="0"), or if it is saturated in all of the 1.3 s "Read 2" Ks-band exposures. |
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Additional Source Quality Information | ||||||
dist_edge_ns | %5d | arcsec | no | The distance from the source to the nearest North or South scan edge. The scan edge is defined by the great-circle interpolation between the 3-band coverage corners. The equatorial coordinates of the 3-band coverage corners are given in the Scan Information Table (NOT YET AVAILABLE), referenced by the scan_key. The first character of the dist_edge_flg indicates to which edge the source is closer. | ||
dist_edge_ew | %3d | arcsec | no | The distance from the source to the nearest East or West scan edge. The scan edge is defined by the great-circle interpolation between the 3-band coverage corners. The equatorial coordinates of the 3-band coverage corners are given in the Scan Information Table (NOT YET AVAILABLE), referenced by the scan_key. The second character of the dist_edge_flg indicates to which edge the source is closer. | ||
dist_edge_flg | %2s | --- | no | Two character flag that specifies to which scan edges a source lies closest, and to which edges the dist_edge_ns and dist_edge_ew values refer. The first character encodes the N/S edge: "n" means that dist_edge_ns refers to north scan edge, "s" means that dist_edge_ns refers to the south scan edge. The second character encodes the E/W edge: "e" means that dist_edge_ew refers to the east scan edge, "w" means that dist_edge_ew refers to the west scan edge. | ||
dup_src | %1d | --- | no | Duplicate source flag. Used in conjunction with the
use_src flag, this numerical flag indicates
whether the source falls in a Tile overlap
region, and if so, if it was detected multiple times.
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use_src | %1d | --- | no | Use source flag. Used in conjunction with the
dup_src flag, this numerical flag indicates
if a source falls within a Tile overlap
region, and whether or not it satisfies the unbiased selection
rules for multiple source resolution.
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Optical Source Association Information | ||||||
a | %1s | --- | no | Catalog identifier of an optical source from either
the Tycho 2 or USNO-A2.0 catalog that falls within
~5" of the 2MASS source position. An association with Tycho 2
takes precedence over USNO-A2.0. The values of this column can be:
Positional association between the 2MASS PSC source and an optical catalog source does not guarantee an identification. Users should consider the separation between the sources, the number of possible optical matches, and consider proper motion when assessing optical counterparts to 2MASS sources. The optical association information is unreliable for sources with |dec|>86° because of an error in the 2MASS/USNO-A2.0 position correlation procedure that caused associations to be missed in the vicinity of the equatorial poles. If the source has |dec|>86°, a value of a="0" does not necessarily mean that there is not an optical association within 5´´ of the 2MASS position. |
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dist_opt | %3.1f | arcsec | yes | Distance separating 2MASS source position and associated optical source within 5". For Tycho 2 associations (a="T"), the separation is computed for the position of the Tycho 2 source corrected for proper motion to the time of the 2MASS observation (if proper motions are provided in Tycho 2). This column is null if there is no associated optical source (a="0"). | ||
phi_opt | %4d | deg | yes | Position angle on the sky of the vector from the the associated optical source to the 2MASS source position, in degrees East of North. This is opposite to the sense of prox which is the vector from the 2MASS source position to the nearest neighbor in the PSC. This column is null if there is no associated optical source (a="0"). | ||
b_m_opt | %5.2f | mag | yes | Blue magnitude of associated optical source. If Tycho 2 (a="T"), then this is the Johnson B magnitude (BJ, derived from BTycho and VTycho using the transformations given in Høg (2000): BJ-VJ = 0.85*(BT-VT). If USNO-A2.0 (a="U"), then this is the photographic blue magnitude. This column is null if there is no associated optical source (a="0"). | ||
vr_m_opt | %5.2f | mag | yes | Visual or red magnitude of the associated optical source. If Tycho 2 (a="T"), then this is the Johnson V magnitude (VJ), derived from BTycho and VTycho using the transformations given in Høg (2000): VJ = VT - 0.09*(BT-VT). If USNO-A2.0 (a="U"), then this is the photographic red magnitude. This column is null if there is no associated optical source (a="0"). | ||
nopt_mchs | %1d | --- | no | The number of USNO-A2.0 or Tycho 2 optical sources found within
a 5" radius of the 2MASS position.
The optical association information is unreliable for sources with |dec|>86° because of an error in the 2MASS/USNO-A2.0 position correlation procedure that caused associations to be missed in the vicinity of the equatorial poles. If the source has |dec|>86°, a value of nopt_mchs=0 does not necessarily mean that there is not an optical association within 5´´ of the 2MASS position. |
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Cross-Index Information | ||||||
ext_key | %7d | --- | yes | Unique identification number of the record in the XSC that corresponds to this point source. The XSC record with this ext_key value will have the pts_key for this source in its pts_key column. This allows easy cross-referencing between the two catalogs. | ||
scan_key | %5d | ---- | no | Unique identification number of the record in the Scan Information Table (NOT YET AVAILABLE) that corresponds to the survey scan in which this source was detected. | ||
coadd_key | %7d | ---- | no | Unique identification number of the record in the Atlas Image Data Table (NOT YET AVAILABLE) that corresponds to Image in which the position of this source falls. | ||
coadd | %3d | ---- | no | Sequence number of the Atlas Image in which the position of this source falls. The Image sequence number is number of the frame that is nearest the center of the Image. |
[Last Updated: 2003 May 16, by R. Cutri]