2024MNRAS.528.3000M


Query : 2024MNRAS.528.3000M

2024MNRAS.528.3000M - Mon. Not. R. Astron. Soc., 528, 3000-3008 (2024/February-3)

Determining cosmological growth parameter for stellar-mass black holes.

MLINAR E. and ZWITTER T.

Abstract (from CDS):

It has recently been suggested that black holes (BHs) may grow with time, so that their mass is proportional to the cosmological scale factor to the power n, with suggested values n ≈ 3 for supermassive BHs in elliptical galaxies. Here, we test these predictions with stellar-mass BHs in X-ray binaries using their masses and ages. We perform two sets of tests to assess the compatible values of n. First, we assume that no compact object grows over the Tolman-Oppenheimer-Volkoff limit which marks the borderline between neutron stars and BHs. We show that half of BHs would be born with a mass below this limit if n = 3 applies. The possibility that all BHs were born above the limit is rejected at $4\, \sigma$ if n = 3 applies. In the second test, we assume that masses of BHs at their formation stay the same over cosmic history. We compare the mass distribution of the youngest BHs, which could have not grown yet, to their older counterparts. Distributions are compatible for $n = -0.9^{+1.3}_{-4.6}$, with n = 3 excluded formally with 87 per cent confidence. This result may be biased, because massive BHs tend to have a massive companion. Correcting for this bias yields n ≈ 0. We can therefore conclude that while our results are not a clear rejection of BH scaling with n = 3, we show that n = 0 is much more consistent with the data.

Abstract Copyright: © 2024 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): binaries: close - stars: black holes - cosmology: theory - X-rays: binaries

Simbad objects: 26

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Number of rows : 26
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 CXOU J005510.0-374212 HXB 00 55 09.990 -37 42 12.16     22.44     WNE 139 1
2 NAME M33 X-7 HXB 01 33 34.13 +30 32 11.3 17.50 18.80 18.70     O 187 2
3 SN 1997D SN* 04 11 01.00 -56 29 56.0       16.3   SNIIpec 184 1
4 2MASS J05380840-6909190 SB* 05 38 08.4066684408 -69 09 18.975749724   15.47 15.26     O7V(n)((f)) 44 0
5 X LMC X-3 HXB 05 38 56.6323605504 -64 05 03.317937504   17 17.2     B2.5Ve 722 0
6 X LMC X-1 HXB 05 39 38.8284304464 -69 44 35.531553624   14.8 14.5 14.924   O8(f)p 700 0
7 1A 0620-00 HXB 06 22 44.5423857312 -00 20 44.290460544           K3V-K7V 1144 0
8 V* MM Vel HXB 10 13 36.3431303106 -45 04 31.128938218           G5V-M0V 211 1
9 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120           K5V-M1V 865 0
10 UCAC4 154-126202 SB* 13 50 16.7477601784 -59 14 20.330701044   13.995 12.711 12.366   ~ 58 0
11 V* BW Cir HXB 13 58 09.7227337579 -64 44 05.257858491           ~ 256 0
12 SNR G323.7-01.0 SNR 15 34 30.1 -57 12 03           ~ 25 0
13 MAXI J1535-571 XB* 15 35 19.73 -57 13 48.1           ~ 214 0
14 V* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760         15.624 ~ 532 1
15 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
16 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
17 NGC 6242 OpC 16 55 31.8 -39 28 09           ~ 98 0
18 MAXI J1659-152 LXB 16 59 01.680 -15 15 28.73           ~ 274 0
19 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
20 GALEX J172841.0-003451 SB* 17 28 41.0966126056 -00 34 51.523377959       13.977   ~ 64 0
21 V* V4641 Sgr HXB 18 19 21.6343259256 -25 24 25.849595952     13.654 13.479 13.139 B9III 530 0
22 MAXI J1820+070 LXB 18 20 21.9423816480 +07 11 07.284859440           ~ 511 0
23 SS 433 HXB 19 11 49.5647697480 +04 58 57.827127648   16.854 14.643     A7Ib 2253 4
24 SNR G039.7-02.0 SNR 19 12 20 +04 55.0           ~ 378 1
25 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
26 V* V404 Cyg HXB 20 24 03.8247037434 +33 52 01.961154861           G9/K0III/V 1370 0

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