Chandra observations of low-mass X-ray binaries and diffuse gas in the early-type galaxies NGC 4365 and NGC 4382 (M85)

被引:48
作者
Sivakoff, GR
Sarazin, CL
Irwin, JA
机构
[1] Univ Virginia, Dept Astron, Charlottesville, VA 22903 USA
[2] Univ Michigan, Dept Astron, Ann Arbor, MI 48109 USA
关键词
binaries : close; galaxies : elliptical and lenticular; cD; galaxies : ISM; X-rays : binaries; X-rays : galaxies; X-rays : ISM;
D O I
10.1086/379115
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We used the Chandra X-Ray Observatory ACIS-S3 to image the X-ray-faint elliptical galaxy NGC 4365 and lenticular galaxy NGC 4382. The observations resolve much of the X-ray emission into 99 and 58 sources, respectively, most of which are low-mass X-ray binaries (LMXBs) associated with each of the galaxies. Within one effective radius of NGC 4365, about 45% of the counts are resolved into sources, 30% are attributed to unresolved LMXBs, and 25% are attributed to diffuse gas. Within two effective radii of NGC 4382, about 22% of the counts are resolved into sources, 33% are attributed to unresolved LMXBs, and 45% are attributed to diffuse gas. We identify 18 out of the 37 X-ray sources in a central field in NGC 4365 with globular clusters. The luminosity functions of the resolved sources for both galaxies are best fitted with cutoff power laws whose cutoff luminosity is approximate to (0.9-3.1) x 10(39) ergs s(-1). These luminosities are much larger than those previously measured for similar galaxies; we do not find evidence for a break in the luminosity function at the Eddington luminosity of a 1.4 M-. neutron star. The spatial distributions of the resolved sources for both galaxies are broader than the distribution of optical stars. In both galaxies, a hard powerlaw model fits the summed spectrum of all of the sources. The unresolved emission is best fitted by the sum of a soft MEKAL model, representing emission from diffuse gas, and a hard power law, presumed to be from unresolved LMXBs. There is some evidence that the temperature of the diffuse gas increases with increasing radius. A standard beta model fits the radial distribution of the diffuse gas in both galaxies. In the elliptical galaxy NGC 4365, the best-fit core radius is very small, while the SO galaxy NGC 4382 has a larger core radius. This may indicate that the gas in NGC 4382 is rotating significantly.
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收藏
页码:218 / 236
页数:19
相关论文
共 40 条
[1]   The X-ray globular cluster population in NGC 1399 [J].
Angelini, L ;
Loewenstein, M ;
Mushotzky, RF .
ASTROPHYSICAL JOURNAL, 2001, 557 (01) :L35-L38
[2]   Bulge-disk decomposition of 659 spiral and lenticular galaxy brightness profiles [J].
Baggett, WE ;
Baggett, SM ;
Anderson, KSJ .
ASTRONOMICAL JOURNAL, 1998, 116 (04) :1626-1642
[3]   Compact group selection from redshift surveys [J].
Barton, E ;
Geller, MJ ;
Ramella, M ;
Marzke, RO ;
daCosta, LN .
ASTRONOMICAL JOURNAL, 1996, 112 (03) :871-&
[4]   Diffuse gas and low-mass X-ray binaries in the Chandra observation of the S0 galaxy NGC 1553 [J].
Blanton, EL ;
Sarazin, CL ;
Irwin, JA .
ASTROPHYSICAL JOURNAL, 2001, 552 (01) :106-119
[5]   Observations of faint, hard-band X-ray sources in the field of CRSS J0030.5+2618 with the Chandra X-Ray Observatory and the Hobby-Eberly Telescope [J].
Brandt, WN ;
Hornschemeier, AE ;
Schneider, DP ;
Garmire, GP ;
Chartas, G ;
Hill, GJ ;
MacQueen, PJ ;
Townsley, LK ;
Burrows, DN ;
Koch, TS ;
Nousek, JA ;
Ramsey, LW .
ASTRONOMICAL JOURNAL, 2000, 119 (05) :2349-2359
[6]   Structure and evolution of interstellar gas in flattened, rotating elliptical galaxies [J].
Brighenti, F ;
Mathews, WG .
ASTROPHYSICAL JOURNAL, 1996, 470 (02) :747-761
[7]   X-ray spectral analysis of elliptical galaxies from ASCA: the Fe abundance in a multiphase medium [J].
Buote, DA ;
Fabian, AC .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 1998, 296 (04) :977-994
[8]   PROPERTIES OF THE X-RAY EMITTING GAS IN EARLY-TYPE GALAXIES [J].
CANIZARES, CR ;
FABBIANO, G ;
TRINCHIERI, G .
ASTROPHYSICAL JOURNAL, 1987, 312 (02) :503-513
[9]  
CUTRI RM, 2001, 2MASS 2 INCREMENTA S
[10]  
DAVIS DS, 1996, APJ, V470, P35