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IPCDEEP - Einstein Catalog IPC Deep Survey |
HEASARC Archive |
Primini, F.A., Murray, S.S., Huchra, J., Schild, R., Burg, R., and Giacconi, R. Imaging X-ray Astronomy, ed. M. Elvis (Cambridge, Cambridge University Press), p. 337. Primini, F.A., Murray, S.S., Huchra, J., Schild, R., Burg, R., and Giacconi, R. 1991, Ap.J., 374, 440.
BII
The galactic longitude of the object.
Broad_Background_Counts
The number of background counts in the detect cell in the broad band. The
background counts are determined either from counts in a region surrounding the
detect cell (LDETECT) or from counts in the corresponding detect cell of the
background map (MDETECT).
Broad_Background_Error
The background counts error in the detect cell in the broad band. In the case
of counts from the background map, the error in the background counts is
assumed to be zero.
Broad_Counts
The number of source counts in the detect cell at the source position for the
broad band (0.16-3.5 keV).
Broad_Counts_Error
The source counts error at the source position for the broad band (0.16-3.5
keV).
Broad_Flux
The broad band flux (in ergs/cm**2/s).
Broad_Flux_Error
The broad band flux error.
Broad_SNR
The broad band signal-to-noise ratios.
Correction_Factor
The deep survey count rate correction factor; this number will be 0 if the
source was excluded from the DSMAP. Otherwise, it will be equal to the ratio of
the livetime of the sequence number to the livetime of the DSMAP. This
correction is necessary because the DSMAP templates used to construct
background maps are generated from the deep survey observations themselves.
Thus calculation of count rates for deep survey sources may be biased by
inclusion of source counts in the background map. Correction for this bias is
described in detail in Primini et al. 1991.
Count_Rate
The broad band corrected count rate (in counts/sec). In general, the corrected
count rate is determined as follows:
Corr Count Rate = (Counts - bkgrd counts) * vign corr * CMS * CPRF / livetime
CPRF corrects for source photons which fall outside the detect cell. Detect cell sizes are chosen so that CPRF=1.13 for all energy bands. CMS corrects for large angle scattering intrinsic in the HEAO-2 mirror. This factor is energy-dependent and has a value of 1.09 for the soft band and 1.18 for the hard and broad bands. For deep survey sources, additional minor count rate corrections may be necessary. These corrections are descripted under Deep Survey Count Rate Correct.
Count_Rate_Error
The broad band corrected count rate error.
Dec
The Declination of the object.
Detect_Method
The detection method and band which describes the origin of the position for
each IPC source detected during standard Rev 1B processing. There are six
combinations which describe the detection method and band for each IPC source
detected; these combinations are given by a two-digit code, with the first
digit representing the detection method (L for L detect, or M for M detect),
and the second digit representing the spectral band used in detection (S for
soft, H for hard, or B for broad). This also describes from which method/band
combination the position is given; it is the first available one from the
following prioritized order: MH, MB, MS, LH, LB, LS.
Hard_Background_Counts
The number of background counts in the detect cell in the hard band. The
background counts are determined either from counts in a region surrounding the
detect cell (LDETECT) or from counts in the corresponding detect cell of the
background map (MDETECT).
Hard_Background_Error
The background counts error in the detect cell in the hard band. In the case
of counts from the background map, the error in the background counts is
assumed to be zero.
Hard_Corr_Count_Rate
The hard band corrected count rate (in counts/sec). In general, the corrected
count rate is determined as follows:
Corr Count Rate = (Counts - bkgrd counts) * vign corr * CMS * CPRF / livetime
CPRF corrects for source photons which fall outside the detect cell. Detect cell sizes are chosen so that CPRF=1.13 for all energy bands. CMS corrects for large angle scattering intrinsic in the HEAO-2 mirror. This factor is energy-dependent and has a value of 1.09 for the soft band and 1.18 for the hard and broad bands. For deep survey sources, additional minor count rate corrections may be necessary. These corrections are descripted under Deep Survey Count Rate Correct.
Hard_Count_Rate_Error
The hard band corrected count rate error.
Hard_Counts
The number of source counts in the detect cell at the source position for the
hard band (0.8-3.5 keV).
Hard_Counts_Error
The source counts error at the source position for the hard band (0.8-3.5 keV).
Hard_Flux
The hard band flux (in ergs/cm**2/s).
Hard_Flux_Error
The hard band flux error.
Hard_SNR
The hard band signal-to-noise ratios.
LII
The galactic latitude of the object.
Name
Name is derived from the concatonation of the Sequence Number and the Source
Number.
Off_Axis_Angle
The off-axis angle, in arcminutes, is the distance of the source from the
pointing position of the observation.
Pos_Code
The position code for each source. The position code will have bit 0 (the
least significant bit) set if the source is within the central 32'x32' of the
field. It will have bit 1 set if Rib Edge code > 0.
Pos_Uncert
The positional uncertainty, in arcseconds.
RA
The Right Ascension of the object.
Rib_Edge_Code
A numeric flag with nonzero values indicating that the detection cell (and/or
frame defined for "local detect") falls near or on a rib shadow or detector
edge. The code is formed by concatenating a pair of two-digit numbers: the
first (thousands and hundreds columns) gives the number (up to 16) of frame
subcells potentially shadowed by the ribs or masked-field edge; the second
(tens and units columns) gives the number of subcells (up to 09) within the
detect box which are potentially shadowed.
Sequence_Num
This gives the Einstein Observatory sequence number, a two to five digit number
which uniquely identifies the observation. The numbers were assigned
sequentially at the time of proposal submission.
Soft_Background_Counts
The number of background counts in the detect cell in the soft band. The
background counts are determined either from counts in a region surrounding the
detect cell (LDETECT) or from counts in the corresponding detect cell of the
background map (MDETECT).
Soft_Background_Error
The background counts error in the detect cell in the soft band. In the case
of counts from the background map, the error in the background counts is
assumed to be zero.
Soft_Corr_Count_Rate
The soft band corrected count rate (in counts/sec). In general, the corrected
count rate is determined as follows:
Corr Count Rate=(Counts - bkgrd counts) * vign corr * CMS * CPRF / livetime
CPRF corrects for source photons which fall outside the detect cell. Detect cell sizes are chosen so that CPRF=1.13 for all energy bands. CMS corrects for large angle scattering intrinsic in the HEAO-2 mirror. This factor is energy-dependent and has a value of 1.09 for the soft band and 1.18 for the hard and broad bands. For deep survey sources, additional minor count rate corrections may be necessary. These corrections are descripted under Deep Survey Count Rate Correct.
Soft_Count_Rate_Error
The soft band corrected count rate error.
Soft_Counts
The number of source counts in the detect cell at the source position in the
soft band (0.16-0.8 keV).
Soft_Counts_Error
The source counts error at the source position in the soft band (0.16-0.8 keV).
Soft_Flux
The soft band flux (in ergs/cm**2/s).
Soft_Flux_Error
The soft band flux error.
Soft_SNR
The soft band signal-to-noise ratios.
Source_Num
The IPC source number within the field.
Vignetting_Correction
The Rev 1B vignetting correction and is used in determining the corrected count
rates.