2021ApJ...912L..31W


Query : 2021ApJ...912L..31W

2021ApJ...912L..31W - Astrophys. J., 912, L31-L31 (2021/May-2)

The pair-instability mass gap for black holes.

WOOSLEY S.E. and HEGER A.

Abstract (from CDS):

Stellar evolution theory predicts a "gap" in the black hole birth function caused by the pair instability. Many presupernova stars that have a core mass below some limiting value, Mlow, after all pulsational activity is finished, collapse to black holes, while more massive ones, up to some limiting value, Mhigh, explode, promptly and completely, as pair-instability supernovae. Previous work has suggested Mlow ≃ 50 M and Mhigh ≃ 130 M. These calculations have been challenged by recent LIGO observations that show many black holes merging with individual masses Mlow >= 65 M. Here we explore four factors affecting the theoretical estimates for the boundaries of this mass gap: nuclear reaction rates, evolution in detached binaries, rotation, and hyper-Eddington accretion after black hole birth. Current uncertainties in reaction rates by themselves allow Mlow to rise to 64 M and Mhigh as large as 161 M. Rapid rotation could further increase Mlow to ∼70 M, depending on the treatment of magnetic torques. Evolution in detached binaries and super-Eddington accretion can, with great uncertainty, increase Mlow still further. Dimensionless Kerr parameters close to unity are allowed for the more massive black holes produced in close binaries, though they are generally smaller.

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): Stellar mass black holes - Core-collapse supernovae - Hypernovae - Gravitational wave astronomy

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 - 2024
#notes
1 * eta Car Em* 10 45 03.545808 -59 41 03.95124 6.37 7.03 6.48 6.123 4.41 LBV 2444 0
2 SS 433 HXB 19 11 49.5647697480 +04 58 57.827127648   16.854 14.643     A3/7I 2126 4
3 GrW 190521 GWE ~ ~           ~ 293 0

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