2022ApJ...938...69P


Query : 2022ApJ...938...69P

2022ApJ...938...69P - Astrophys. J., 938, 69 (2022/October-2)

On the Mass Function of GWTC-2 Binary Black Hole Systems and Their Progenitors.

PARK H.-J., KIM S.-J., KIM S. and VAN PUTTEN M.H.P.M.

Abstract (from CDS):

The distribution of LIGO black hole binaries (BBH) shows an intermediate-mass range consistent with the Salpeter initial mass function (IMF) in black hole formation by core-collapse supernovae, subject to preserving binary association. They are effectively parameterized by the mean mass μ with a Pearson correlation coefficient of r = 0.93 ± 0.06 of secondary to primary masses with a mean mass ratio of $\bar{q}\simeq 0.67$, q = M2/M1, consistent with the paucity of intermediate-mass X-ray binaries. The mass function of LIGO BBHs is well approximated by a broken power law with a tail μ ≳ 31.4 M⊙ in the mean binary mass $\mu =\left({M}_{1}+{M}_{2}\right)/2$. Its power-law index of αB,true = 4.77 ± 0.73 inferred from the tail of the observed mass function is found to approach the upper bound 2αS = 4.7 of the uncorrelated binary IMF, defined by the Salpeter index αS = 2.35 of the IMF of stars. The observed low scatter in BBH mass ratio q evidences equalizing mass transfer in binary evolution prior to BBH formation. At the progenitor redshift ${z}^{{\prime} }$, furthermore, the power-law index satisfies ${\alpha }_{B}^{{\prime} }\gt {\alpha }_{B}$ in a flat ΛCDM background cosmology. The bound ${\alpha }_{B,\mathrm{true}}^{{\prime} }\lesssim 2{\alpha }_{S}$ hereby precludes early formation at arbitrarily high redshifts ${z}^{{\prime} }\gg 1$, which may be made more precise and robust with extended BBH surveys from upcoming LIGO O4-5 observations.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Astrophysical black holes

Simbad objects: 6

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Number of rows : 6
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 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
3 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
4 GrW 150914 GWE ~ ~           ~ 674 1
5 GRB 190425 GWE ~ ~           ~ 438 0
6 GrW 190521 GWE ~ ~           ~ 409 0

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