Astronomical Data Center

ADCADC/CDS Standard Document for Catalog:
/external/photom/E2005/

The ADC has expanded its resources in order to better serve our users, we have developed a new category called "external" to complement our catalogs and journal table directories.
You can access the incremental data release 2 (March 2000) version of the data set described here through the URL:
http://adc.gsfc.nasa.gov/cgi-bin/adc/cat.pl?/B/2mass.
or
You can access the home site of the data set described here through the URL:
http://www.ipac.caltech.edu/2mass/overview/access.html.

The following is an abbreviated "ReadMe" document that describes this external data set.
E/II/5                      The 2MASS database                (IPAC/UMass, 2000)
================================================================================
The Two Micron All Sky Survey
    Skrutskie M.F., Schneider S.E., Stiening R., Strom S.E., Weinberg M.D., 
    Beichman C., Chester T., Cutri R., Lonsdale C.,
    Elias J., Elston R., Capps R., Carpenter J., Huchra J., 
    Liebert J., Monet D., Price S., Seitzer P.
   <Proc. Workshop "The Impact of Large Scale Near-IR Sky Surveys", 25 (1997)>
================================================================================
ADC_Keywords: Infrared sources ; Photometry, infrared ; Surveys; 
              External catalog

Location: http://www.ipac.caltech.edu/2mass/overview/access.html

Description:
    The Two Micron All Sky Survey (2MASS) project is designed to close the
    gap between our current technical capability and our knowledge of the
    near-infrared sky. In addition to providing a context for the
    interpretation of results obtained at infrared and other wavelengths,
    2MASS will provide direct answers to immediate questions on the
    large-scale structure of the Milky Way and the Local Universe.

    To achieve these goals, 2MASS is uniformly scanning the entire sky in
    three near-infrared bands to detect and characterize point sources
    brighter than about 1 mJy in each band, with signal-to-noise ratio
    (SNR) greater than 10, using a pixel size of 2.0". This will achieve
    an 80,000-fold improvement in sensitivity relative to earlier surveys.

    2MASS uses two new, highly-automated 1.3-m telescopes, one at Mt.
    Hopkins, AZ, and one at CTIO, Chile. Each telescope is equipped with a
    three-channel camera, each channel consisting of a 256x256 array of
    HgCdTe detectors, capable of observing the sky simultaneously at J
    (1.25 {mu}m), H (1.65 {mu}m), and Ks (2.17 {mu}m), to a 3{sigma}
    limiting sensivity of 17.1, 16.4 and 1.3mag in thge three bands.

    The 2MASS arrays image the sky while the telescopes scan smoothly in
    declination at a rate of ~1' per second. The 2MASS data "tiles" are
    6{deg} long in the declination direction and one camera frame (8.5')
    wide. The camera field-of-view shifts by ~1/6 of a frame in
    declination from frame-to-frame. The camera images each point on the
    sky six times for a total integration time of 7.8 s, with sub-pixel
    "dithering", which improves the ultimate spatial resolution of the
    final Atlas Images.

    The University of Massachusetts (UMass) is responsible for the overall
    management of the project, and for developing the infrared cameras and
    on-site computing systems at both facilities. The Infrared Processing
    and Analysis Center (IPAC) is responsible for all data processing
    through the Production Pipeline, and construction and distribution of
    the data products. The 2MASS project involves the participation of
    members of the Science Team from several different institutions. The
    2MASS project is funding by the National Aeronautics and Space
    Administration (NASA) and the National Science Foundation (NSF).

File Summary:
--------------------------------------------------------------------------------
 FileName   Lrecl    Records    Explanations
--------------------------------------------------------------------------------
ReadMe         80          .    This file
out.sam       292       1000    2MASS Point Source Catalogue, sample output,
                                 incremental data release 2 (March 2000). 
--------------------------------------------------------------------------------

See also:
    http://www.ipac.caltech.edu/2mass/ : 2MASS documentation

Nomenclature Notes:
    As specified by the IAU recommendations on source nomenclature, the
    object designation is derived from the J2000 sexagesimal coordinates
    of the source and has the form HHMMSSS+/-DDMMSS, where HH are the
    hours of right ascension, MM the RA minutes and SSS are the
    deci-seconds of RA; DD are the degrees in declination, MM are DEC
    minutes and SS the declination seconds. Note that both the RA
    deci-seconds of time and DEC seconds of arc are truncated rather than
    rounded, per the IAU recommendation.

    It was discovered that about 100,000 objects have non-unique source
    designations; a column f_Name was added to flag those objects which
    name appears more than once in the survey.

Byte-by-byte Description of output: out.sam
--------------------------------------------------------------------------------
  Bytes Format Units    Label     Explanations
--------------------------------------------------------------------------------
   1- 10  F10.6 deg     RAdeg     Right ascension (J2000)
  12- 21  F10.6 deg     DEdeg     Declination (J2000)
  23- 26  F4.2  arcsec  MajAxis   ? Major axis of position error ellipse
  28- 31  F4.2  arcsec  MinAxis   ? Minor axis of position error ellipse
  34- 36  I3    deg     Theta     [0,180]? Position angle of error ellipse 
                                  major axis (E of N)
  38- 38  A1    ---   f_Name      [* ] A '*' flags a non-unique source
                                  designation
  39- 52  A14   ---     Name      Source designation
--------------------------------------------------------------------------------
  54- 60  F7.3  mag     Jmag      ?=-99.999 J selected "default" magnitude (1)
  62- 66  F5.3  mag   e_Jmag_d    ? J "default" magnitude uncertainty (2)
  68- 72  F5.3  mag   e_Jmag      ? J "total" magnitude uncertainty (3)
  74- 80  F7.3  mag     Hmag      ?=-99.999 H selected "default" magnitude (1)
  82- 86  F5.3  mag   e_Hmag_d    ? H "default" magnitude uncertainty (2)
  88- 92  F5.3  mag   e_Hmag      ? H "total" magnitude uncertainty (3)
  94-100  F7.3  mag     Kmag      ?=-99.999 K selected "default" magnitude (1)
 102-106  F5.3  mag   e_Kmag_d    ? Ks "default" magnitude uncertainty (2)
 108-112  F5.3  mag   e_Kmag      ? Ks "total" magnitude uncertainty (3)
--------------------------------------------------------------------------------
 114-116  A3    ---     rd_flg    [012348] Source of JHK "default" mag (4)
 119-121  A3    ---     bl_flg    [012] JHK components fit to source (5)
 124-126  A3    ---     cc_flg    [UNPCDSRGB0] Artifact contamin./confusion (6)
     131  I1    ---     extd_flg  [0,2]? Extended source contamination (7)
     133  I1    ---     mp_flg    [0,1]? Association with asteroid or comet (8)
--------------------------------------------------------------------------------
     138  A1    ---     Id_opt    [UT] Associated optical source (9)
 140-144  F5.2  mag     Bmag      ? Blue mag of associated optical source
 146-150  F5.2  mag     Rmag      ? Red mag of associated optical source
 153-156  F4.2  arcsec  Dist_opt  ? Distance to associated optical source
 159-161  I3    deg     PAopt     [0,360]?  position angle to optical source
 165-166  I2    ---     Nopt_mchs ? Number of optical sources within 5 arcsec
--------------------------------------------------------------------------------
#169-178  A10 "MM/DD/YYYY" Date   Observation date
 169-178  A10   ---     Date      Observation date
     183  A1    ---     Hemis     [ns] Hemisphere of observation
 186-188  I3    ---     Scan      ? Scan number (within date)
 190-195  I6    ---     Id        Source id number (within scan)
 197-206  F10.6 deg     GLON      Galactic longitude
 208-217  F10.6 deg     GLAT      Galactic latitude
 219-224  F6.2  ---     Jpsfchi   ? J band reduced chi2 value of fit
 226-231  F6.2  ---     Hpsfchi   ? H band reduced chi2 value of fit
 233-238  F6.2  ---     Kpsfchi   ? K band reduced chi2 value of fit
--------------------------------------------------------------------------------
 240-246  F7.3  mag     Jm_stdap  ? J standard or BF aperture magnitude (10)
 248-253  F6.3  mag   e_Jm_stdap  ? error on J_m_stdap
 255-261  F7.3  mag     Hm_stdap  ? H standard or BF aperture magnitude (10)
 263-268  F6.3  mag   e_Hm_stdap  ? error on H_m_stdap
 270-276  F7.3  mag     Km_stdap  ? K standard or BF aperture magnitude (10)
 278-283  F6.3  mag   e_Km_stdap  ? error on K_m_stdap
--------------------------------------------------------------------------------
 287-292  A6    ---     Ndet_flg  [0-9 ] Number of aperture measurements 
                                         (jjhhkk) (11)
--------------------------------------------------------------------------------
Note (1): This is the selected "default" magnitude for each band
    (centered at J: 1.25, H: 1.65 and Ks: 2.17{mu}m).
    For most sources, the [jhk]_m values are the PSF fit mags for each
    band (rd_flg=2). If the source has a null PSF-fit magnitude but a
    valid std. aperture magnitude in a band, the [jhk]_m value for that
    band is the std. aperture magnitude (rd_flg=4). If the source is
    saturated in R2-R1 in a band, but not saturated in the R1 exposure,
    the default magnitude is the R1 aperture magnitude (rd_flg=1). If the
    source is saturated in even the R1 exposure (rd_flg=3) or if the
    source is a bright star placeholder (rd_flg=8), the default magnitude
    is given as -99.999. Finally, if a source is band-filled in a band,
    the value of [jhk]_m for that band is the band-fill 95%-confidence
    upper limit mag (rd_flg=0).

    This value is computed as follows:

        Lim95 = integrated flux + (2 * noise) 

    where the noise in this case means the "local noise", computed as
    follows (using the DAOPHOT algorithm):

        noise = sqrt(error1 + error2 + error3) 
    where

        error1 = variance in the local sky 
               = npix * skyvar 
          npix = number of pixels in the aperture 
        skyvar = the variance of the sky brightness 
        error2 = photon noise 
               = int. flux * Gain 
        error3 = (skyvar/nsky) * (npix ** 2) 
          nsky = number pixels in sky annulus 
    (skyvar/nsky) = square of the standard error of the mean sky brightness 

    For the case in which the integrated flux is negative, the upper limit
    is
        Lim95 = 2 * noise 
    where
        noise = sqrt(error1 + error3) 

Note (2): The mag sigma values corresponding to the selected "default" 
    magnitude for each band are put in the [jhk]_msig fields. For
    non-detections (band-fills), the mag sigmas are null. An unphysically
    large magnitude sigma value (e.g. >0.36) indicates that the source was
    detected in that band, but either the brightness measurement
    encountered problems due to confusion or other contamination, or the
    detection is of very low confidence. Objects that are saturated in R1
    in any band have magnitude sigmas of 9.999.

Note (3): The "combined" uncertainty in the quoted magnitude for each band 
    that provides an estimate of all random errors that contribute to the
    photometric uncertainty. This uncertainty is the quadratic combination
    of the extraction uncertainites ([jhk]_msig), and the photometric zero
    point offset uncertainties from the night during which the source was
    observed ([jhk]_zperr from the "Scan Data" table), and the residual
    flat-fielding errors (estimated to be 0.005 mags for all bands). For
    R1 sources, the quadratic sum includes the RMS uncertainty in the
    normalization of the R1 photometry to the R2-R1 photometry
    ([jhk]_r1normrms from the "Scan Data" table).

Note (4): The read flag indicates the source of J,H,K "default" magnitudes
    as a 3-digit integer, where the 1st digit corresponds to the J band,
    the 2nd to the H band, and the 3rd to the Ks band. The values are as
    follows:
    0: source is not detected in this band (is band-filled)
    1: default mag is R1 aperture
    2: default mag is R2-R1 profile-fit
    3: default magnitude is -99.999. Source is saturated in R1.
    4: default mag is R2-R1 standard aperture mag
    8: default magnitude is -99.999. Source is "placeholder" for a very 
       bright star heavily saturated in R1. Position information derived 
       from Positions and Proper Motions Star Catalogue (Roser and Bastian,
       1991, See Catalogues <I/146>, <I/193>, <I/208>).

Note (5): The "blend" flag indicates how many point source components 
    were fit to each band's source during the profile fitting process. It
    is a 3-digit integer, where each digit can be 
       0: source not detected in band, 
       1: single profile fit to isolated source, or 
       2: multiple sources detected abd fit simultaneously
    The 1st digit corresponds to the J band, the 2nd to the H band, and
    the 3rd to the Ks band.

Note (6): The contamination/confusion flag indicates whether the 
    source's photometry and position may be affected by artifacts of
    nearby bright stars or by confusion with other nearby sources. The
    flag consists of a 3 character string, where the 1st character
    corresponds to the J band, the 2nd to the H band, and the 3rd to the
    Ks band.

    Sources are tested for contamination and/or confusion in the order
    given below, and once a flag is applied to the source, testing is
    stopped in that band. The flag values indicate the source may be:

    U: unreliable source. Most likely a spurious detection of a meteor
       trail or a noise excursion
    N: photometric normalization problem due to the influence of a very
       bright star in the scan. Photometry in this band may be as much as
       1 magnitude offset from the correct value
    P: affected by a nearby persistence artifact
    D: affected by a nearby diffraction spike
    S: affected by a horizontal "stripe" artifact (due to a bright star) 
    R: affected by a nearby bright star reflection artifact
    C: affected by confusion with another nearby source
    B: affected by confusion in bandmerging
    0: default value -- not contaminated or not detected in the band

Note (7): The "extended" flag is set to 
    0 if the point source is not associated with an extended source, 
    1 if it is identically associated with an object in the extended 
      source catalog (e.g. the nucleus of a galaxy), or 
    2 if it is simply contaminated by an extended source (e.g. a star 
      superimposed on the disk of a galaxy).

Note (8): This object is positionally associated with the location of 
    a known minor planet or comet at the time of the 2MASS observation.
    See the table of known asteroid and comet detections for more
    information.

Note (9): The catalog ID and other association parameters are given for 
    the closest optical match found within 5 arcsec. The ID consists of a
    single-letter abbreviation for the catalog: 
    'T' for Tycho-ACT (see Cat. <I/246>)
    'U' for USNO-A (see Cat. I/252>)

Note (10): If a source is not detected in a band (band-filled), 
    this field in that band contains the band-filled aperture-photometry
    mag. It is calculated by measuring the brightness within an 8"
    diameter aperture at the position of the source on the Atlas Image:

        BFMag = ZERO_CAL - 2.5 log10(flux) 

    where ZERO_CAL is the zero calibration magnitude. Note that this field
    may have to represent a negative flux; in such a case, the value is:

        BFMag = 99.0 - [ZERO_CAL - 2.5 log10(|flux|)] 

    This encoding requires fluxes close to zero to be clipped. The
    clipping distance is set to 0.01 DN above zero for positive fluxes and
    below zero for negative fluxes. For example, the positive flux 0.0005
    DN would be clipped at 0.01 DN and encoded as:

        BFMag = ZERO_CAL - 2.5 log10(0.01) 
              = 24.93 (for ZERO_CAL = 19.93) 

    For a negative flux of -0.0005 DN, the clipping would yield -0.01 DN,
    and the encoding would be

        BFMag = 99.0 - [ZERO_CAL - 2.5 log10(0.01)] 
              = 74.07 (for ZERO_CAL = 19.93) 

    BFMags near 50 cannot occur, so 50 marks the boundary between positive
    and negative flux encoding.

Note (11): This flag consists of 6 single-digit numbers, 
    two digits per band in the order JJHHKK. 
    The 1st digit for each band indicates the number of frames with 
        >3-sigma aperture mag measurements, and 
    the 2nd digit indicates the number of frames in which aperture 
        measurements were possible. (This flag is AKA the 
        N-out-of-M statistic).
--------------------------------------------------------------------------------

Important Notice:

    Please include the following in any published material that makes use
    of the 2MASS data products:

    "This publication makes use of data products from the Two Micron All
    Sky Survey, which is a joint project of the University of
    Massachusetts and the Infrared Processing and Analysis Center, funded
    by the National Aeronautics and Space Administration and the National
    Science Foundation."

History:
  * 07-Sep-2000: first version of 2nd Incremental Data Release
  * 19-Mar-2001: added f_Name column which flags non-unique source names.
================================================================================
(End)                 Sebastien Derriere, Francois Ochsenbein [CDS]  07-Sep-2000

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