High-mass binary black hole mergers from detailed binary evolution models
arXiv:2607.27962
The paper uses detailed binary evolution simulations to test whether super‑Eddington mass transfer in isolated binaries can produce the observed high‑mass binary black hole mergers, finding that fully‑conservative accretion is disfavored and that additional formation channels are likely needed.
Abstract
Gravitational-wave observations reveal a population of binary black hole (BBH) mergers with primary masses above , extending into and potentially beyond the pair-instability mass gap, with a possibly flat mass-ratio and broader Ï_\mathrm{eff} distribution. We investigate whether super-Eddington accretion during stable mass transfer in isolated binary evolution can produce BBH mergers consistent with these properties across primary BH mass, mass-ratio, and Ï_\mathrm{eff} distributions. Using POSYDON, we simulate BBH merger populations with primary BH masses above , under three BH accretion efficiencies: Eddington-limited, GRRMHD-informed, and fully conservative. We additionally vary the natal kick strength, including strong kicks at high BH masses. We find that super-Eddington accretion does not suppress BBH mergers in the high-mass regime. Fully-conservative accretion leads to an increase of BBH mergers in POSYDON with a strong kick-independent peak at and a sharp mass-ratio peak at , whereas observations favor and a flatter mass-ratio distribution. The GRRMHD-informed and Eddington-limited accretion are compatible with the observed primary BH mass and mass ratio distribution, but require natal kicks to populate negative Ï_\mathrm{eff}. A joint analysis of the primary BH mass, mass ratio, and Ï_\mathrm{eff} distributions provides strong constraints on binary evolution physics, and disfavor fully-conservative BH accretion as the dominant formation mechanism for high-mass BBH mergers. The Eddington-limited and GRRMHD-informed prescriptions with modest kicks can explain part of the high-mass population, but an additional formation channel is still needed to account for the high fraction of negative Ï_\mathrm{eff} systems and high secondary BH spins.
Submitted to ApJ. Comments welcome