2004ApJ...612..848H


Query : 2004ApJ...612..848H

2004ApJ...612..848H - Astrophys. J., 612, 848-859 (2004/September-2)

A Chandra view of the normal S0 galaxy NGC 1332. I. An unbroken, steep power-law luminosity function for the low-mass X-ray binary population.

HUMPHREY P.J. and BUOTE D.A.

Abstract (from CDS):

Chandra ACIS -S3 observations of the nearby S0 galaxy NGC 1332 resolve much of the X-ray emission into 73 point sources, of which 37 lie within the D25isophote. The remaining galaxy emission comprises hot, diffuse gas and unresolved sources and is discussed in two companion papers. The point-source X-ray luminosity function (XLF) shows the characteristic break seen in other early-type galaxies at ∼2x1038 ergs/s. After applying corrections for detection incompleteness at low luminosities due to source confusion and contamination from diffuse galactic emission, the break vanishes and the data are well described as a single power law. This result casts further doubt on there being a ``universal'' XLF break in early-type galaxies, marking the division between neutron star and black hole systems. The logarithmic slope of the differential XLF (dN/dL), β=2.7±0.5, is marginally (∼2.5 σ) steeper than has been found for analogous completeness-corrected fits of other early-type galaxies but closely matches the behavior seen at high luminosities in these systems. Two of the sources within D25 are ultraluminous X-ray sources (ULXs), although neither have LX>2x1039 ergs/s. The absence of very luminous ULXs in early-type galaxies suggests a break in the XLF slope at ~(1-2)x1039 ergs/s, although the data were not of sufficient quality to constrain such a feature in NGC 1332. The sources have a spatial distribution consistent with the optical light and display a range of characteristics that are consistent with an LMXB population. The general spectral characteristics of the individual sources, as well as the composite source spectra, are in good agreement with observations of other early-type galaxies, although a small number of highly absorbed sources are seen. Two sources have very soft spectra, two show strong variability, indicating compact binary nature, and one source shows evidence of an extended radial profile. We do not detect a central source in NGC 1332, but we find a faint [LX=(2±1)x1038 ergs/s] point source coincident with the center of the companion dwarf galaxy NGC 1331.

Abstract Copyright:

Journal keyword(s): Galaxies: Elliptical and Lenticular, cD - Galaxies: Individual: NGC Number: NGC 1332 - X-Rays: Binaries - X-Rays: Galaxies

VizieR on-line data: <Available at CDS (J/ApJ/612/848): table1.dat>

Nomenclature: Table 1: [HB2004] NN (Nos 1-73).

Simbad objects: 82

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Number of rows : 82
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 12650 1
2 2E 0150.5-1358 ClG 01 53 00.40 -13 44 18.0           ~ 387 0
3 NGC 720 Sy1 01 53 00.523 -13 44 19.25   12.4   10.36   ~ 522 0
4 NGC 1316 BL? 03 22 41.789 -37 12 29.52 9.81 9.15 8.53 7.66   ~ 1387 1
5 CXOU J032601.6-212021 X 03 26 01.6 -21 20 21           ~ 1 0
6 CXOU J032601.7-211726 X 03 26 01.7 -21 17 26           ~ 1 0
7 CXOU J032602.2-212140 X 03 26 02.2 -21 21 40           ~ 1 0
8 CXOU J032603.1-211921 X 03 26 03.1 -21 19 21           ~ 1 0
9 CXOU J032604.4-212258 X 03 26 04.4 -21 22 58           ~ 1 0
10 CXOU J032604.7-211613 X 03 26 04.7 -21 16 13           ~ 1 0
11 CXOU J032605.7-212058 X 03 26 05.7 -21 20 58           ~ 1 0
12 CXOU J032606.7-212139 X 03 26 06.7 -21 21 39           ~ 1 0
13 CXOU J032606.8-212016 X 03 26 06.8 -21 20 16           ~ 1 0
14 CXOU J032607.9-211828 X 03 26 07.9 -21 18 28           ~ 1 0
15 CXOU J032609.2-212156 X 03 26 09.2 -21 21 56           ~ 1 0
16 CXOU J032609.7-212211 X 03 26 09.7 -21 22 11           ~ 1 0
17 CXOU J032610.3-211842 X 03 26 10.3 -21 18 42           ~ 1 0
18 CXOU J032612.5-212342 X 03 26 12.5 -21 23 42           ~ 1 0
19 CXOU J032612.8-212000 XB* 03 26 12.8 -21 20 00           ~ 2 0
20 CXOU J032613.1-212020 XB* 03 26 13.1 -21 20 20           ~ 2 0
21 CXOU J032613.9-211944 XB* 03 26 13.9 -21 19 44           ~ 2 0
22 CXOU J032613.9-212005 XB* 03 26 13.9 -21 20 05           ~ 2 0
23 CXOU J032614.2-211950 XB* 03 26 14.2 -21 19 50           ~ 2 0
24 CXOU J032614.6-211955 XB* 03 26 14.6 -21 19 55           ~ 2 0
25 CXOU J032614.6-211903 X 03 26 14.6 -21 19 03           ~ 1 0
26 CXOU J032614.8-212126 X 03 26 14.8 -21 21 26           ~ 1 0
27 CXOU J032615.2-212001 XB* 03 26 15.2 -21 20 01           ~ 2 0
28 CXOU J032615.2-211924 XB* 03 26 15.2 -21 19 24           ~ 2 0
29 CXOU J032615.4-211948 XB* 03 26 15.4 -21 19 48           ~ 2 0
30 CXOU J032615.5-211941 XB* 03 26 15.5 -21 19 41           ~ 2 0
31 CXOU J032615.7-212017 XB* 03 26 15.7 -21 20 17           ~ 2 0
32 2MASS J03261572-2120385 XB* 03 26 15.7508157480 -21 20 38.188417920           ~ 2 0
33 CXOU J032616.2-211953 XB* 03 26 16.2 -21 19 53           ~ 2 0
34 CXOU J032616.3-211958 XB* 03 26 16.3 -21 19 58           ~ 2 0
35 CXOU J032616.4-211953 XB* 03 26 16.46 -21 19 51.3           ~ 2 0
36 CXOU J032616.5-211920 XB* 03 26 16.5 -21 19 20           ~ 2 0
37 CXOU J032616.6-211927 XB* 03 26 16.6 -21 19 27           ~ 2 0
38 CXOU J032616.7-211954 XB* 03 26 16.7 -21 19 54           ~ 3 0
39 CXOU J032616.9-212006 XB* 03 26 16.9 -21 20 06           ~ 2 0
40 CXOU J032617.1-212011 X 03 26 17.1 -21 20 11           ~ 1 0
41 NGC 1332 GiP 03 26 17.321 -21 20 07.33   11.45   9.84   ~ 350 0
42 CXOU J032617.6-212013 XB* 03 26 17.67 -21 20 11.6           ~ 2 0
43 CXOU J032618.1-212014 XB* 03 26 18.1 -21 20 14           ~ 3 0
44 CXOU J032618.3-212011 XB* 03 26 18.31 -21 20 09.4           ~ 2 0
45 CXOU J032618.7-212031 XB* 03 26 18.7 -21 20 31           ~ 2 0
46 CXOU J032618.7-211814 X 03 26 18.7 -21 18 14           ~ 1 0
47 CXOU J032618.8-212148 X 03 26 18.8 -21 21 48           ~ 1 0
48 CXOU J032619.0-212030 XB* 03 26 19.0 -21 20 30           ~ 2 0
49 CXOU J032619.3-212052 XB* 03 26 19.3 -21 20 52           ~ 2 0
50 CXOU J032619.4-212021 XB* 03 26 19.35 -21 20 18.8           ~ 2 0
51 CXOU J032619.9-212019 XB* 03 26 19.9 -21 20 19           ~ 2 0
52 CXOU J032620.0-212023 XB* 03 26 20.0 -21 20 23           ~ 2 0
53 CXOU J032620.1-211958 XB* 03 26 20.1 -21 19 58           ~ 2 0
54 CXOU J032620.4-212112 XB* 03 26 20.4 -21 21 12           ~ 2 0
55 CXOU J032620.5-212041 XB* 03 26 20.5 -21 20 41           ~ 2 0
56 CXOU J032620.6-212317 X 03 26 20.6 -21 23 17           ~ 1 0
57 CXOU J032620.6-211713 X 03 26 20.6 -21 17 13           ~ 1 0
58 CXOU J032620.7-212151 X 03 26 20.7 -21 21 51           ~ 1 0
59 CXOU J032620.8-211957 X 03 26 20.8 -21 19 57           ~ 1 0
60 CXOU J032621.5-212029 XB* 03 26 21.53 -21 20 27.9           ~ 2 0
61 CXOU J032621.6-211930 X 03 26 21.6 -21 19 30           ~ 1 0
62 CXOU J032621.8-211930 X 03 26 21.8 -21 19 30           ~ 1 0
63 CXOU J032621.9-212023 XB* 03 26 21.9 -21 20 23           ~ 2 0
64 CXOU J032622.4-212132 X 03 26 22.4 -21 21 32           ~ 1 0
65 CXOU J032622.6-212418 X 03 26 22.6 -21 24 18           ~ 1 0
66 CXOU J032622.8-211917 X 03 26 22.8 -21 19 17           ~ 1 0
67 CXOU J032622.8-211620 X 03 26 22.8 -21 16 20           ~ 1 0
68 CXOU J032623.1-211945 X 03 26 23.1 -21 19 45           ~ 1 0
69 CXOU J032624.2-212040 XB* 03 26 24.2 -21 20 40           ~ 2 0
70 CXOU J032625.1-212043 XB* 03 26 25.1 -21 20 43           ~ 2 0
71 CXOU J032625.5-211622 X 03 26 25.5 -21 16 22           ~ 1 0
72 CXOU J032627.4-212235 X 03 26 27.4 -21 22 35           ~ 1 0
73 NGC 1331 GiG 03 26 28.3322458080 -21 21 19.955101860   14.25   12.86   ~ 76 0
74 CXOU J032630.9-211824 X 03 26 30.9 -21 18 24           ~ 1 0
75 CXOU J032631.3-212339 X 03 26 31.3 -21 23 39           ~ 1 0
76 CXOU J032631.3-212210 X 03 26 31.3 -21 22 10           ~ 1 0
77 CXOU J032632.8-212306 X 03 26 32.8 -21 23 06           ~ 1 0
78 CXOU J032634.7-211755 X 03 26 34.7 -21 17 55           ~ 1 0
79 CXOU J032636.5-211809 X 03 26 36.5 -21 18 09           ~ 1 0
80 NGC 4038 EmG 12 01 53.002 -18 52 03.32   10.91   9.74 11.0 ~ 1333 1
81 NAME Antennae IG 12 01 53.170 -18 52 37.92           ~ 1692 0
82 NGC 4039 GiP 12 01 53.51 -18 53 10.3   11.08   9.77   ~ 1161 1

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