2004ApJ...611..846K


Query : 2004ApJ...611..846K

2004ApJ...611..846K - Astrophys. J., 611, 846-857 (2004/August-3)

X-ray luminosity function and total luminosity of low-mass X-ray binaries in early-type galaxies.

KIM D.-W. and FABBIANO G.

Abstract (from CDS):

We have derived bias-corrected X-ray luminosity functions (XLFs) of sources detected in a uniformly selected sample of 14 E and S0 galaxies observed with Chandra ACIS-S3. The entire sample yields 985 pointlike X-ray sources, with typical detections of 30-140 sources per galaxy. After correcting for incompleteness, the individual XLFs are statistically consistent with a single power law of a (differential) XLF slope β=1.8-2.2 (with a typical error of 0.2-0.3). A break at or near LX,Edd, as reported in the literature for some of these galaxies, is not required in any case. Given the uniform XLF shape, we have generated a combined, higher statistics XLF, representative of X-ray sources in elliptical galaxies. Although the combined XLF is marginally consistent with a single power law (with β=2.1±0.1), a broken power law gives an improved fit. The best-fit slope is β=1.8±0.2 in the low-luminosity range LX=afewx1037 to 5x1038 ergs/s. At higher luminosities, the slope is steeper, β=2.8±0.6. The break luminosity is (5±1.6)x1038 ergs/s (with an error at 90%), which may be consistent with the Eddington luminosity of neutron stars with the largest possible mass (3 M☉), He-enriched neutron star binaries, or low-mass stellar-mass black holes. If the change in XLF slope at high luminosities is real and does not mask a step in the XLF, our result would imply a different population of high-luminosity sources, instead of a beaming effect. This high-luminosity portion of the XLF must reflect the mass function of black holes in these galaxies. We note that this high-luminosity population does not resemble that of the ultraluminous X-ray sources detected in star-forming galaxies, where no break in the XLF is present and the XLF is much flatter than in the older stellar system we are studying here. We use our results to derive the integrated X-ray luminosity of accreting low-mass X-ray binaries (LMXBs) in each sample galaxy. We confirm that the total X-ray luminosity of LMXBs is correlated with the optical and more tightly with the near-IR luminosities, but in both cases the scatter exceeds that expected from measurement errors. We find that the scatter in LX(LMXB)/LKis marginally correlated with the specific frequency of globular clusters.

Abstract Copyright: ∼

Journal keyword(s): Galaxies: Elliptical and Lenticular, cD - X-Rays: Binaries - X-Rays: Galaxies

Simbad objects: 19

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Number of rows : 19
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
2 BAX 028.2522-13.7387 ClG 01 53 00.40 -13 44 18.0           ~ 389 0
3 NGC 720 Sy1 01 53 00.523 -13 44 19.25   12.4   10.36   ~ 536 0
4 NGC 1316 rG 03 22 41.789 -37 12 29.52 9.81 9.15 8.53 7.66   ~ 1491 1
5 NGC 1399 rG 03 38 29.083 -35 27 02.67 11.05 9.74 9.59 8.12   ~ 1636 1
6 ACO S 373 ClG 03 38 29.4 -35 27 08           ~ 2029 0
7 NGC 1407 rG 03 40 11.904 -18 34 49.36   10.64 9.67 9.13   ~ 613 2
8 M 105 LIN 10 47 49.600 +12 34 53.87   10.56 9.76 9.12 8.18 ~ 1504 0
9 NGC 4365 GiG 12 24 28.228 +07 19 03.07   11.5       ~ 871 0
10 M 84 Sy2 12 25 03.74333 +12 53 13.1393 12.67 12.09 10.49     ~ 1841 2
11 M 85 GiP 12 25 24.053 +18 11 27.89   10.2       ~ 678 0
12 M 49 Sy2 12 29 46.8 +08 00 01   13.21 12.17     ~ 2174 2
13 NAME Virgo Cluster ClG 12 30 47.8 +12 23 07           ~ 7107 0
14 M 59 GiG 12 42 02.2581375168 +11 38 48.909507756   11.0       ~ 721 0
15 NAME NGC 4636 Group GrG 12 42 49.5 +02 41 08           ~ 570 0
16 NGC 4636 LIN 12 42 49.8333280080 +02 41 15.951929028   12.62 11.84     ~ 1156 1
17 M 60 GiC 12 43 39.9708251934 +11 33 09.688174067   10.3       ~ 1395 1
18 NGC 4697 GiG 12 48 35.8981498824 -05 48 02.482374564   10.97   9.83   ~ 895 0
19 IC 1459 rG 22 57 10.60682195 -36 27 43.9966421   10.96 11.85 9.34 10.3 ~ 652 2

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