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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