2023NatAs...7.1090B


Query : 2023NatAs...7.1090B

2023NatAs...7.1090B - Nature Astronomy, 7, 1090-1097 (2023/September-0)

The formation of merging black holes with masses beyond 30 M⊙ at solar metallicity.

BAVERA S.S., FRAGOS T., ZAPARTAS E., ANDREWS J.J., KALOGERA V., BERRY C.P.L., KRUCKOW M., DOTTER A., KOVLAKAS K., MISRA D., ROCHA K.A., SRIVASTAVA P.M., SUN M. and XING Z.

Abstract (from CDS):

Gravitational-wave astronomy has revealed a population of stellar-mass black holes more massive than observed previously by other means. The maximum mass of black holes formed in isolated binaries is determined by stellar winds, mixing processes and interactions between the binary components. We consider the impact that fully self-consistent, detailed stellar-structure and binary-evolution calculations have on the population synthesis of black-hole binaries at solar metallicity. We find a qualitatively different picture from previous studies employing rapid population-synthesis techniques. Merging binary black holes form with a non-negligible rate (∼4×10-7M-1⊙∼4×10-7M⊙-1∼4×1{0}^{-7} {M}_☉^{-1}) and their progenitor stars with initial masses ≳50 M⊙ do not expand to supergiant radii, thereby largely avoiding substantial dust-driven or luminous blue variable winds. The progenitor stars lose less mass in winds, which results in black holes as massive as ∼30 M⊙, and approximately half avoid a mass-transfer episode before forming the first-born black hole. Binaries with initial periods of a few days, some of which may undergo Roche-lobe overflow mass transfer, result in mildly spinning first-born black holes, χBH1 ≲ 0.2, assuming efficient angular-momentum transport.


Abstract Copyright: 2023 The Author(s), under exclusive licence to Springer Nature Limited

Journal keyword(s):

Simbad objects: 3

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Number of rows : 3
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 GrW 190814 GWE 00 55.8 -27 05           ~ 433 0
2 MAXI J1631-479 XB? 16 31 14.06 -47 48 25.6           ~ 56 0
3 GrW 150914 GWE ~ ~           ~ 674 1

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