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NARCSCAT - Norma Arm Region Chandra Survey Point & Extended Source Catalog |
HEASARC Archive |
Chandra ACIS-I observations were performed in faint mode of a 2 degree by 0.8 degree region of the Norma spiral arm in 2011 June. This field was subdivided into 27 pointings; Table 1 in the reference paper reports their coordinates and exposure times and Figure 1 (op. cit.) is a mosaic image of the survey. The observing strategy was to cover a wide area with relatively uniform flux sensitivity and good spatial resolution; therefore, the authors chose field centers spaced by 12 arcminutes, which provided roughly 70 arcminute2 of overlap on the outskirts of adjacent observations such that the additional exposure time in these overlapping regions partly made up for the worsening point-spread function (PSF) at large off-axis angles.
The Norma Arm Region Chandra Survey Catalog: X-Ray Populations in the Spiral Arms. Fornasini F.M., Tomsick J.A., Bodaghee A., Krivonos R.A., An Hongjun, R.F., Gotthelf E.V., Bauer F.E., Stern D. <Astrophys. J., 796, 105. (2014)> =2014ApJ...796..105F
Source_Number
A uniquely identifying source number for each Chandra X-ray
source in this catalog, in order on increasing J2000.0 Right Ascension.
Name
The standard (with the exception noted below) Chandra X-ray source
designation recommended by the Dictionary of Nomenclature of Celestial
Objects, viz., the 'CXOU' prefix for 'Chandra X-Ray Observatory,
Unregistered' combined with the J2000 positional coordinates for the X-ray
source, e.g., 'CXOU J163228.2-473755'. The X-ray sources numbered 172 and 173
have the same positions in this table, as #172 is an extended source
surrounding the point source #173. So as to avoid having duplicate names for
these 2 sources, the HEASARC has given them (unofficial) source suffixes of
'E' and 'P', respectively: thus, source #172 is now named 'CXOU
J163447.8-473243E' and source #173 is now named 'CXOU J163447.8-473243P'.
ObsID_1
The Chandra observation identifier (ObsID) of a Chandra pointing in which
wavdetect detected the source. The list of 27 Chandra pointings from which
this catalog is derived is given in Table 1 of the reference paper. Since
these pointings overlapped, a given source could be detected in more than
pointing. See Section 2.1 of the reference paper for the details about
wavdetect usage.
ObsID_2
The Chandra observation identifier (ObsID) of a Chandra pointing in which
wavdetect detected the source. The list of 27 Chandra pointings from which
this catalog is derived is given in Table 1 of the reference paper. Since
these pointings overlapped, a given source could be detected in more than
pointing. See Section 2.1 of the reference paper for the details about
wavdetect usage.
ObsID_3
The Chandra observation identifier (ObsID) of a Chandra pointing in which
wavdetect detected the source. The list of 27 Chandra pointings from which
this catalog is derived is given in Table 1 of the reference paper. Since
these pointings overlapped, a given source could be detected in more than
pointing. See Section 2.1 of the reference paper for the details about
wavdetect usage.
RA
The Right Ascension of the X-ray source in the selected equinox. This was
given in J2000 decimal degrees to a precision of 10-6 degrees in the
original table. If the source is detected in multiple observations, the
position reported is the weighted average of its positions in different
observations.
Dec
The Declination of the X-ray source in the selected equinox. This was given
in J2000 decimal degrees to a precision of 10-6 degrees in the original
table. If the source is detected in multiple observations, the position
reported is the weighted average of its positions in different observations.
LII
The Galactic Longitude of the X-ray source.
BII
The Galactic Latitude of the X-ray source.
Error_Radius
The positional uncertainty of the source, in arcseconds. For a source
detected in a given observation, this uncertainty is equal to the quadrature
sum of the 95% statistical uncertainty based on Equation (5) of Hong et al.
(2005, ApJ, 635, 907) and the average systematic uncertainty of the positions
in that observation after astrometric refinement (see Column 5 in Table 2 of
the reference paper). For sources detected in multiple observations, the
uncertainties associated with the source position in different observations
were combined to provide the uncertainty of the weighted average of the
source positions.
Off_Axis_1
The offset angular separation of the source from the center
of the aim point of the observation, in arcminutes, as specified by the
corresponding ObsID, i.e., as given by the obsid_1 parameter value.
Off_Axis_2
The offset angular separation of the source from the center
of the aim point of the observation, in arcminutes, as specified by the
corresponding ObsID, i.e., as given by the obsid_2 parameter value.
Off_Axis_3
The offset angular separation of the source from the center
of the aim point of the observation, in arcminutes, as specified by the
corresponding ObsID, i.e., as given by the obsid_3 parameter value.
FB_Significance
The significance of the X-ray source in the full 0.5 - 10 keV band. It is
calculated by finding the probability that the source is a noise fluctuation
using Equation (5) of the reference paper and using the Gaussian cumulative
distribution function to determine the corresponding source significance. If
the source is detected in multiple observations, the reported significance is
the sum in quadrature of the source significance in the individual
observations.
SB_Significance
The significance of the X-ray source in the soft 0.5 - 2 keV band. It is
calculated by finding the probability that the source is a noise fluctuation
using Equation (5) of the reference paper and using the Gaussian cumulative
distribution function to determine the corresponding source significance. If
the source is detected in multiple observations, the reported significance is
the sum in quadrature of the source significance in the individual
observations.
HB_Significance
The significance of the X-ray source in the hard 2 - 10 keV band. It is
calculated by finding the probability that the source is a noise fluctuation
using Equation (5) of the reference paper and using the Gaussian cumulative
distribution function to determine the corresponding source significance. If
the source is detected in multiple observations, the reported significance is
the sum in quadrature of the source significance in the individual
observations.
Extraction_Radius_1
The radius of the aperture source region, in arcseconds, in the Chandra
observation of the source specified in the obsid_1 parameter. For most
sources, the aperture source region is defined as a circle with a radius
equal to the 90% enclosed-count fraction (ECF) for 4.5 keV photons, i.e., the
point-spread function (PSF) radius. For potentially extended sources, flagged
with a value of 'e' in the corresponding source_flags parameter, the radius
is instead equal to the semi-major axis of the aperture region defined by
wavdetect. In cases where two or more sources have overlapping circular
regions, the regions are redefined as a circular core plus an annular pie
sector following the guidelines in Table 6 of the reference paper; in such
cases, the radius provided in the catalog represents the outer radius of the
pie sector.
Extraction_Radius_2
The radius of the aperture source region, in arcseconds, in the Chandra
observation of the source specified in the obsid_2 parameter. For most
sources, the aperture source region is defined as a circle with a radius
equal to the 90% enclosed-count fraction (ECF) for 4.5 keV photons, i.e., the
point-spread function (PSF) radius. For potentially extended sources, flagged
with a value of 'e' in the corresponding source_flags parameter, the radius
is instead equal to the semi-major axis of the aperture region defined by
wavdetect. In cases where two or more sources have overlapping circular
regions, the regions are redefined as a circular core plus an annular pie
sector following the guidelines in Table 6 of the reference paper; in such
cases, the radius provided in the catalog represents the outer radius of the
pie sector.
Extraction_Radius_3
The radius of the aperture source region, in arcseconds, in the Chandra
observation of the source specified in the obsid_3 parameter. For most
sources, the aperture source region is defined as a circle with a radius
equal to the 90% enclosed-count fraction (ECF) for 4.5 keV photons, i.e., the
point-spread function (PSF) radius. For potentially extended sources, flagged
with a value of 'e' in the corresponding source_flags parameter, the radius
is instead equal to the semi-major axis of the aperture region defined by
wavdetect. In cases where two or more sources have overlapping circular
regions, the regions are redefined as a circular core plus an annular pie
sector following the guidelines in Table 6 of the reference paper; in such
cases, the radius provided in the catalog represents the outer radius of the
pie sector.
PSF_Radius_1
The PSF radius for the 90% ECF for 4.5 keV photons at the
detector location of the source, in arcseconds, in the Chandra observation of
the source specified in the obsid_1 parameter. The PSF radius varies with
detector position, generally increasing with increasing offset angle from the
observation aim point.
PSF_Radius_2
The PSF radius for the 90% ECF for 4.5 keV photons at the
detector location of the source, in arcseconds, in the Chandra observation of
the source specified in the obsid_2 parameter. The PSF radius varies with
detector position, generally increasing with increasing offset angle from the
observation aim point
PSF_Radius_3
The PSF radius for the 90% ECF for 4.5 keV photons at the
detector location of the source, in arcseconds, in the Chandra observation of
the source specified in the obsid_3 parameter. The PSF radius varies with
detector position, generally increasing with increasing offset angle from the
observation aim point
Source_Flags_1
This parameter contains flags for the specified source
in the Chandra observation of the source specified in the obsid_1 parameter,
as follows:
Flag Meaning b 'blended': blended source that is unblended in another observation. c 'created': source noticed by eye but not detected by wavdetect. The source aperture region was created manually based on the visible position and extent of the source. The positional uncertainties calculated for such sources underestimate the true uncertainties, since the source is found by eye and not by wavdetect. e 'extended': possibly extended source. The semi-major axis of the smallest aperture region defined by wavdetect for such sources is larger than twice the PSF radius reported in the corresponding psf_radius_1 parameter. These sources are typically detected in images that have been binned by 4 x 4 or 8 x 8 pixels. id 'inspected duplicate': possible duplicate source flagged for manual inspection. A 'duplicate' source refers to a single source detected in multiple overlapping observations;sources were considered to be duplicates of one another if the distance between them was smaller than the quadrature sum of their positional uncertainties. Sources were flagged for manual inspection if (1) they were separated by a distance greater than the quadrature sum of their positional uncertainties but smaller than the simple sum of their positional uncertainties, or (2) they were separated by a distance smaller than the quadrature sum of their positional uncertainties but differed in a substantial way (e.g., one is flagged as possibly extended while another is not, one is found to have two duplicates by the distance criterion but these two duplicates of the first source are not found to be duplicates of one another by the distance criterion). Generally, if sources flagged with 'id' showed consistent photon fluxes and quantile parameters, they were determined to be true duplicates. m1, m2, 'modified': in cases where the circular source aperture region or m3 overlaps with the aperture region of another source, the source region is modified to reduce overlapping. See Table 6 of the reference paper for details. nb 'near bright': source near a very bright source which may be a spurious detection. nd 'not detected': source is located where at least two observations overlap but it is only detected in one observation s 'surrounding': a possibly extended source that completely surrounds one or more point sources. The aperture regions of the surrounded sources are excluded from the aperture region of the source flagged with an 's' value. vl 'variable long': source determined to be variable on long (hours to days) timescales. The photon flux in at least one energy band (full, soft, or hard) varies by >= 3 sigma between different observations. vp 'variable probable': source is probably variable on short (second to hour) timescales. The K-S test finds the source light curve within a single observation to be inconsistent with a constant light curve at a 95% confidence level. vs 'variable short': source determined to be variable on short (seconds to hours) timescales. The K-S test finds the source light curve within a single observation to be inconsistent with a constant light curve at a >= 3-sigma confidence level.
Source_Flags_2
This parameter contains flags for the specified source
in the Chandra observation of the source specified in the obsid_2 parameter,
with the same possible values and meanings as given for the source_flags_1
parameter (see above).
Source_Flags_3
This parameter contains flags for the specified source
in the Chandra observation of the source specified in the obsid_3 parameter,
with the same possible values and meanings as given for the source_flags_1
parameter (see above).
FB_Counts_Limit
This parameter is set to '<' if the corresponding counts
value is an upper limit rather than an actual detection in this band.
FB_Counts
The net source counts in the full 0.5-10 keV band, calculated as described in
Section 2.2 of the reference paper.For cases in which the estimated
background counts in a source aperture region were determined to be greater
than or equal to the total number of counts in the source region, then the
catalog presents the 90% upper confidence limit to the net source counts
based on the method described in Kraft et al. (1991, ApJ, 374, 344); in such
cases, the corresponding error parameters are left blank and the
corresponding limit value set to '<'. For sources detected in multiple
observations, the net counts from different observations were added together.
FB_Counts_Pos_Err
The upper 1-sigma error for the net full 0.5-10 keV band
source counts. For sources detected in multiple observations, the errors are
combined in quadrature.
FB_Counts_Neg_Err
The lower 1-sigma error for the net full 0.5-10 keV band
source counts. For sources detected in multiple observations, the errors are
combined in quadrature.
SB_Counts_Limit
This parameter is set to '<' if the corresponding counts
value is an upper limit rather than an actual detection in this band.
SB_Counts
The net source counts in the soft 0.5-2 keV band, calculated as described in
Section 2.2 of the reference paper.For cases in which the estimated
background counts in a source aperture region were determined to be greater
than or equal to the total number of counts in the source region, then the
catalog presents the 90% upper confidence limit to the net source counts
based on the method described in Kraft et al. (1991, ApJ, 374, 344); in such
cases, the corresponding error parameters are left blank and the
corresponding limit value set to '<'. For sources detected in multiple
observations, the net counts from different observations were added together.
SB_Counts_Pos_Err
The upper 1-sigma error for the net soft 0.5-2 keV band
source counts. For sources detected in multiple observations, the errors are
combined in quadrature.
SB_Counts_Neg_Err
The lower 1-sigma error for the net soft 0.5-2 keV band
source counts. For sources detected in multiple observations, the errors are
combined in quadrature.
HB_Counts_Limit
This parameter is set to '<' if the corresponding counts
value is an upper limit rather than an actual detection in this band.
HB_Counts
The net source counts in the hard 2-10 keV band, calculated as described in
Section 2.2 of the reference paper.For cases in which the estimated
background counts in a source aperture region were determined to be greater
than or equal to the total number of counts in the source region, then the
catalog presents the 90% upper confidence limit to the net source counts
based on the method described in Kraft et al. (1991, ApJ, 374, 344); in such
cases, the corresponding error parameters are left blank and the
corresponding limit value set to '<'. For sources detected in multiple
observations, the net counts from different observations were added together.
HB_Counts_Pos_Err
The upper 1-sigma error for the net hard 2-10 keV band
source counts. For sources detected in multiple observations, the errors are
combined in quadrature.
HB_Counts_Neg_Err
The lower 1-sigma error for the net hard 2-10 keV band
source counts. For sources detected in multiple observations, the errors are
combined in quadrature.
FB_Photon_Flux_Limit
This parameter is set to '<' if the corresponding
photon flux value is an upper limit rather than an actual detection in this
band.
FB_Photon_Flux
The photon flux of the Chandra source in the full 0.5-10 keV
band, in photons cm-2 s-1. The photon flux was calculated by dividing
the net counts by the exposure time and the mean effective area within the
source region. For sources with zero or negative net counts, the catalog
provides the 90% upper limit on the photon flux, the corresponding error
parameters are left blank and the corresponding limit value is set to '<'. For
sources detected in multiple observations, the average photon fluxes are
reported; if a source was found to be variable between observations (flagged
with a value of 'vl' in the source_flags parameter), then its photon fluxes
from individual observations were simply averaged, but otherwise its photon
fluxes were weight-averaged.
FB_Photon_Flux_Pos_Err
The upper 1-sigma error in the net full 0.5-10 keV
band photon flux, in photons cm-2 s-1.
FB_Photon_Flux_Neg_Err
The lower 1-sigma error in the net full 0.5-10 keV
band photon flux, in photons cm-2 s-1.
SB_Photon_Flux_Limit
This parameter is set to '<' if the corresponding
photon flux value is an upper limit rather than an actual detection in this
band.
SB_Photon_Flux
The photon flux of the Chandra source in the soft 0.5-2 keV
band, in photons cm-2 s-1. The photon flux was calculated by dividing
the net counts by the exposure time and the mean effective area within the
source region. For sources with zero or negative net counts, the catalog
provides the 90% upper limit on the photon flux, the corresponding error
parameters are left blank and the corresponding limit value is set to '<'. For
sources detected in multiple observations, the average photon fluxes are
reported; if a source was found to be variable between observations (flagged
with a value of 'vl' in the source_flags parameter), then its photon fluxes
from individual observations were simply averaged, but otherwise its photon
fluxes were weight-averaged.
SB_Photon_Flux_Pos_Err
The upper 1-sigma error in the net soft 0.5-2 keV
band photon flux, in photons cm-2 s-1.
SB_Photon_Flux_Neg_Err
The lower 1-sigma error in the net soft 0.5-2 keV
band photon flux, in photons cm-2 s-1.
HB_Photon_Flux_Limit
This parameter is set to '<' if the corresponding
photon flux value is an upper limit rather than an actual detection in this
band.
HB_Photon_Flux
The photon flux of the Chandra source in the hard 2-10 keV
band, in photons cm-2 s-1. The photon flux was calculated by dividing
the net counts by the exposure time and the mean effective area within the
source region. For sources with zero or negative net counts, the catalog
provides the 90% upper limit on the photon flux, the corresponding error
parameters are left blank and the corresponding limit value is set to '<'. For
sources detected in multiple observations, the average photon fluxes are
reported; if a source was found to be variable between observations (flagged
with a value of 'vl' in the source_flags parameter), then its photon fluxes
from individual observations were simply averaged, but otherwise its photon
fluxes were weight-averaged.
HB_Photon_Flux_Pos_Err
The upper 1-sigma error in the net hard 2-10 keV
band photon flux, in photons cm-2 s-1
HB_Photon_Flux_Neg_Err
The lower 1-sigma error in the net hard 2-10 keV
band photon flux, in photons cm-2 s-1.
Median_Energy
The median energy of the source, in keV. It is determined
from the total counts (not background-corrected) in the source region. For
sources detected in multiple observations, the simple average of the energies
from individual observations is reported if a source is found to be variable
between observations or the weighted-average is reported otherwise.
Median_Energy_Error
The 1-sigma error in the median source energy, in keV.
Q25_Energy
The energy below which 25% of the total source counts reside, in
keV. For sources detected in multiple observations, the simple average of the
energies from individual observations is reported if a source is found to be
variable between observations or the weighted-average is reported otherwise.
Q25_Energy_Error
The 1-sigma error in the energy below which 25% of the
total source counts reside, in keV.
Q75_Energy
The energy below which 75% of the total source counts reside, in
keV. For sources detected in multiple observations, the simple average of the
energies from individual observations is reported if a source is found to be
variable between observations or the weighted-average is reported otherwise.
Q75_Energy_Error
The 1-sigma error in the energy below which 75% of the
total source counts reside, in keV.
FB_Flux_Limit
This parameter is set to '<' if the corresponding full band
flux value is an upper limit rather than an actual detection.
FB_Flux
The energy flux of the source in the full 0.5-10 keV band, in
erg cm-2 s-1. This estimate of the energy flux is calculated by multiplying
the full-band photon flux and the median energy of the source provided in the
catalog. In cases where only an upper limit to the photon flux is available,
the 90% upper limit to the energy flux is reported herein, the error
parameter value is left blank, and the corresponding limit value is set to '<'.
FB_Flux_Pos_Err
The upper 1-sigma error in the net full band 0.5-10 keV
band energy flux, in erg cm-2 s-1.
FB_Flux_Neg_Err
The lower 1-sigma error in the net full band 0.5-10 keV
band energy flux, in erg cm-2 s-1.
Photometric_Flags
This parameter contains photometric flags which
indicate the presence of non-detections in some of the energy bands. If the
photometric values provided for a source are 90% upper limits in the full,
soft, and/or hard energy bands, this column displays an 'F', 'S', and/or 'H',
respectively.
Quantile_Group
The spectral group ('A', B', 'C', 'D' or 'E') defined using
quantile diagrams to which the source belongs. See Section 3 (particularly
Figure 8) of the reference paper for the full details about the quantile
analysis and the significance of the spectral groups defined in this work.
VVV_Source
The source number of the nearest VISTA Variables in the Via
Lactea (VVV: Minniti et al. 2010, NewA, 14, 433) Survey infrared source to the
Chandra source position, if there is one within the 3-sigma uncertainty.
IR_RA
The Right Ascension of the infrared source counterpart in the
selected equinox. This was given in J2000 decimal degrees to a precision of
10-6 degrees in the original table.
IR_Dec
The Declination of the infrared source counterpart in the
selected equinox. This was given in J2000 decimal degrees to a precision of
10-6 degrees in the original table.
Xray_IR_Offset
The angular separation between the Chandra and VVV source positions, in
arcseconds.
IR_Noise_Probability
The probability that the VVV infrared source counterpart is a noise
fluctuation, as provided in the VVV Catalog.
IR_Match_Reliability
The reliability of the VVV counterpart calculated according to the method of
Sutherland & Saunders (1992, MNRAS, 259, 413). The reliability depends on the
angular distance between the X-ray and IR sources, the positional
uncertainties of the X-ray and IR sources, and the spatial density of IR
sources. The reliability is expressed as a fraction between zero and one; VVV
sources with a higher reliability are more likely to be true IR counterparts
to the Chandra sources.