2011ApJ...741..103F


Query : 2011ApJ...741..103F

2011ApJ...741..103F - Astrophys. J., 741, 103 (2011/November-2)

The mass distribution of stellar-mass black holes.

FARR W.M., SRAVAN N., CANTRELL A., KREIDBERG L., BAILYN C.D., MANDEL I. and KALOGERA V.

Abstract (from CDS):

We perform a Bayesian analysis of the mass distribution of stellar-mass black holes using the observed masses of 15 low-mass X-ray binary systems undergoing Roche lobe overflow and 5 high-mass, wind-fed X-ray binary systems. Using Markov Chain Monte Carlo calculations, we model the mass distribution both parametrically–as a power law, exponential, Gaussian, combination of two Gaussians, or log-normal distribution–and non-parametrically–as histograms with varying numbers of bins. We provide confidence bounds on the shape of the mass distribution in the context of each model and compare the models with each other by calculating their relative Bayesian evidence as supported by the measurements, taking into account the number of degrees of freedom of each model. The mass distribution of the low-mass systems is best fit by a power law, while the distribution of the combined sample is best fit by the exponential model. This difference indicates that the low-mass subsample is not consistent with being drawn from the distribution of the combined population. We examine the existence of a "gap" between the most massive neutron stars and the least massive black holes by considering the value, M1%, of the 1% quantile from each black hole mass distribution as the lower bound of black hole masses. Our analysis generates posterior distributions for M1%; the best model (the power law) fitted to the low-mass systems has a distribution of lower bounds with M1%>4.3 M with 90% confidence, while the best model (the exponential) fitted to all 20 systems has M1%>4.5 M with 90% confidence. We conclude that our sample of black hole masses provides strong evidence of a gap between the maximum neutron star mass and the lower bound on black hole masses. Our results on the low-mass sample are in qualitative agreement with those of Ozel et al., although our broad model selection analysis more reliably reveals the best-fit quantitative description of the underlying mass distribution. The results on the combined sample of low- and high-mass systems are in qualitative agreement with Fryer & Kalogera, although the presence of a mass gap remains theoretically unexplained.

Abstract Copyright:

Journal keyword(s): methods: data analysis - X-rays: binaries

Simbad objects: 20

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Number of rows : 20
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 CXOU J002029.1+591651 HXB 00 20 29.09 +59 16 51.9           ~ 170 0
2 CXOU J005510.0-374212 HXB 00 55 09.990 -37 42 12.16     22.44     WNE 126 1
3 NAME M33 X-7 HXB 01 33 34.13 +30 32 11.3 17.50 18.80 18.70     O 164 2
4 V* V518 Per HXB 04 21 42.7227473352 +32 54 26.939156184 13.00 13.50 13.2     M4.5V 651 1
5 X LMC X-1 HXB 05 39 38.8284304464 -69 44 35.531553624   14.8 14.5     O8(f)p 640 2
6 ACO 620 ClG 08 05 44.68 +45 41 44.6           ~ 22 0
7 V* MM Vel HXB 10 13 36.4108035720 -45 04 32.553865524   14.84 14.71     G5V-M0V 198 0
8 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120     12.25     K5V-M1V 822 0
9 V* GU Mus HXB 11 26 26.5961559600 -68 40 32.877752952           K3V-K7V 715 1
10 V* BW Cir HXB 13 58 09.700 -64 44 05.80 17.90 18.00 16.9     ~ 237 1
11 V* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760     11.96     ~ 493 1
12 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000   17.95 16.6     K3III 1172 0
13 [GHJ2008] 3 HXB 16 50 00.980 -49 57 43.60     11.89     K4V 397 0
14 V* V1033 Sco HXB 16 54 00.137 -39 50 44.90   15.20 14.2 16.14   F5IV 1886 1
15 V* V2107 Oph HXB 17 08 14.520 -25 05 30.15   16.50 15.9     K3V-K7V 226 1
16 V* V4641 Sgr HXB 18 19 21.6343259256 -25 24 25.849595952     13.654   13.092 B9III 472 1
17 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2627 0
18 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4334 0
19 V* QZ Vul HXB 20 02 49.58 +25 14 11.3   19.64 18.2     K3V-K6V 421 0
20 V* V404 Cyg HXB 20 24 03.8254458776 +33 52 01.962185735           G9/K0III/V 1275 0

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