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M81CXO - M 81 Chandra X-Ray Discrete Source Catalog |
HEASARC Archive |
The primary X-ray data set is a 49926 s observation of M81 obtained on 2000 May 7 with the Chandra Advanced CCD Imaging Spectrometer (ACIS) spectroscopy array operating in imaging mode. The X-ray data were reprocessed by the Chandra X-ray Center (CXC) on 2001 January 4. These reprocessed data were used in this work. There are no significant differences between the reprocessed data and the originally distributed data analyzed by Tennant et al. (2001ApJ...549L..43T). The observation was taken in faint timed exposure mode at 3.241 s/frame at a focal plane temperature of -120 C. Standard CXC processing has applied aspect corrections and compensated for spacecraft dither.
The primary target, SN 1993J, was located near the nominal aimpoint on the back-illuminated (BI) device S3. The nucleus of M81 lies 2.79' from SN 1993J toward the center of S3 in this observation. Accurate positions of these two objects and two G0 stars located on device S2 were used to identify any offset and to determine absolute locations of the remaining Chandra sources as well as objects in other X-ray images and those obtained at other wavelengths. No offset correction was applied to the Chandra X-ray positions.
Chandra X-ray observations of the spiral galaxy M81. Swartz D.A., Ghosh K.K., McCollough M.L., Pannuti T.G., Tennant A.F., Wu K. <Astrophys. J. Suppl. Ser. 144, 213 (2003)> =2003ApJS..144..213S
Source_Number
A running number for the X-ray source in order of increasing J2000.0 Right
Ascension. #
Name
The name of the X-ray source using the '[SGM2003]' prefix followed by
the X-ray source number, as recommended by the CDS Dictionary of Nomenclature
of Celestial Objects.
RA
The Right Ascension of the X-ray source in the selected equinox. This
was given in J2000.0 coordinates to a precision of 0.01 seconds of time in
the original table.
Dec
The Declination of the X-ray source in the selected equinox. This was
given in J2000.0 coordinates to a precision of 0.1 arcseconds in the original
table.
LII
The Galactic Longitude of the X-ray source.
BII
The Galactic Latitude of the X-ray source.
Count_Rate
The aperture-corrected X-ray source count rate in the ~0.2 to
8.0 keV band, in ct/s.
Count_Rate_Error
The uncertainty in the X-ray source count rate, in ct/s.
SNR
The signal-to-noise ratio of the X-ray source detection.
Vmag_Limit
This parameter is set to '>' to indicate that a counterpart to
the X-ray source was not detected in the V band.
Vmag
The apparent visual magnitude of the counterpart to the X-ray source
derived from either Hubble Space Telescope (HST) WFPC2 images or from the
Perelmutter & Racine (1995, AJ, 109, 1055) catalog of bright objects.
Objects within the 3-sigma uncertainty of the X-ray source positions were
considered potential counterparts to the X-ray sources.
The HST F555W, F606W, or F547M filter measurements and values
have not been corrected for charge transfer efficiency (CTE) effects
nor color-corrected to obtain true Johnson V magnitudes.
Vmag_Flag
This flag parameter has the following possible values:
H = located within HST field but without an optical candidate, implying fainter than the HST limiting magnitude of ~27 magnitudes. I = only F814W (I-band) image available
ACIS_CCD
The Chandra ACIS CCD chip on which the X-ray source was
detected.
Region_Code
The M 81 global environment of the X-ray source position,
coded thus: "b" denotes bulge, "d" denotes disk, and "D_25_" denotes that
the source is outside the D25 isophote.
Lx
The unabsorbed luminosity LX of the source in the 0.3 - 8.0 keV energy
range, in erg/s. For 33 bright sources, this was obtained from the best-fit
spectral models as described below. The luminosities for the remaining
sources were estimated assuming an absorbed power-law spectrum with photon
index Gamma = 1.5 and a hydrogen column density NH = 11.0 x 1020 cm-2.
These are the average values for the 31 of 33 bright sources whose spectra
were best fitted with a power-law model. The source detection limit of 12
counts corresponds to an observed flux of F(0.3-8 keV) = 1.9 x 10-15 erg
cm-2 s-1 for sources on the s3 chip (F(0.3-8 keV) = 2.5 x 10-15 erg
cm-2 s-1 on the FI chips) or an unabsorbed 0.3 - 8 keV luminosity of LX
= 3.4(4.5) x 1036 erg s-1 for sources on the BI (FI) chips.
Lx_Error
The uncertainty in the X-ray luminosity, in erg/s.
The quoted errors are 90% confidence limits for a single interesting parameter
based on the chi-squared fit statistic.
Comments
Additional comments on the source, such as corresponding
X-ray detections from Einstein (denoted "X", Fabbiano, 1988ApJ...325..544F,
sources named '[F88] X-NN' in Simbad) and ROSAT ("P" and "H" denoting PSPC-
and HRI-identified sources, respectively, Immler & Wang, 2001, CDS Cat.
<J/ApJ/554/202>, sources named '[IW2001] PNN' and '[IW2001] HNN' in Simbad),
and potential source types based on spatial correlations with
catalogued objects or on other information (SSS means in Swartz et
al., 2002ApJ...574..382S). Explanations of the quantitative entries are
given in the text of the reference paper.
NH
The best-fit absorption equivalent Hydrogen column density, NH, in H atoms
cm-2, for the X-ray source. The absorption column densities were
constrained in the fitting procedure to be at least as large as the Galactic
column density along the line of sight to M 81. This resulted in a best-fit
value of NH equal to this lower limit for eight sources. Therefore, the
column densities are listed as NH = (4.0 +/- 0.0) x 1020 cm-2 for these
sources.
NH_Error
The RMS uncertainty in the best-fit column density, in cm-2.
The quoted errors are 90% confidence limits for a single interesting parameter
based on the chi-squared fit statistic.
Spect_Index
The best-fit power-law photon index, Gamma, of the X-ray source
spectrum, except for source numbers 160 and 161, where the listed spectral
parameter is the blackbody temperature, kT, in keV. Statistically constrained
model fits could be achieved for a total of 39 sources in the M 81 field.
Detailed X-ray properties of SN 1993J, Einstein source X6, and the nucleus are
presented in Section 4 of the reference paper and of the three brightest
supersoft sources in Swartz et al. (2002, ApJ, 574, 382). The best-fit
spectral model parameters for the remaining 33 bright sources are presented
here. The power-law model provided a significantly better fit to all but the
two X-ray sources listed above.
Spect_Index_Error
The RMS uncertainty in the value of the spectral
parameter. The quoted errors are 90% confidence limits for a single
interesting parameter based on the chi-squared fit statistic.
Chi_Squared
The chi-squared value of the best spectral fit to the X-ray
source spectrum.
DoF
The number of degrees of Freedom of the spectral fit.
Prob_Constant
The Kolmogorov-Smirnov statistic, PKS, used to test the
X-ray sources (including background) for constant count rates over the
duration of the primary observation, in percent. Sources with a low value
of PKS have a high probability of being variable.