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We study the impact of stellar cooling due to light axion emission on the formation and evolution of black hole binaries, via stable mass transfer and the common envelope scenario.~We find that in the presence of light axion emission, no binary black hole mergers are formed with black holes in the lower mass gap ($$M_{\rm BH} < 4 {\rm M}_\odot $$) via the common envelope formation channel.~In some systems, this happens because axions prevent Roche lobe overflow.~In others, they prevent the common envelope from being ejected.~Our results apply to axions with couplings $$ g_{a \gamma} \gtrsim 10^{-10}\, \rm GeV^{-1}$$ (to photons) or $$\alpha_{ae} \gtrsim 10^{-26} $$ (to electrons) and masses $$ m_a \ll 10 \, \rm keV$$.~Light, weakly coupled particles may therefore apparently produce a mass gap $$2 {\rm M}_\odot < M_{\rm BH} < 4 {\rm M}_\odot$$ in the LIGO/Virgo/KAGRA data, when no mass gap is present in the stellar remnant population.
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The Redshift Evolution of the Binary Black Hole Merger Rate: A Weighty Matter
Abstract Gravitational-wave detectors are starting to reveal the redshift evolution of the binary black hole (BBH) merger rate, R BBH ( z ). We make predictions for R BBH ( z ) as a function of black hole mass for systems originating from isolated binaries. To this end, we investigate correlations between the delay time and black hole mass by means of the suite of binary population synthesis simulations, COMPAS . We distinguish two channels: the common envelope (CE), and the stable Roche-lobe overflow (RLOF) channel, characterized by whether the system has experienced a common envelope or not. We find that the CE channel preferentially produces BHs with masses below about 30 M ⊙ and short delay times ( t delay ≲ 1 Gyr), while the stable RLOF channel primarily forms systems with BH masses above 30 M ⊙ and long delay times ( t delay ≳ 1 Gyr). We provide a new fit for the metallicity-dependent specific star formation rate density based on the Illustris TNG simulations, and use this to convert the delay time distributions into a prediction of R BBH ( z ). This leads to a distinct redshift evolution of R BBH ( z ) for high and low primary BH masses. We furthermore find that, at high redshift, R BBH ( z ) is dominated by the CE channel, while at low redshift, it contains a large contribution (∼40%) from the stable RLOF channel. Our results predict that, for increasing redshifts, BBHs with component masses above 30 M ⊙ will become increasingly scarce relative to less massive BBH systems. Evidence of this distinct evolution of R BBH ( z ) for different BH masses can be tested with future detectors.
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- Award ID(s):
- 2009131
- PAR ID:
- 10342642
- Date Published:
- Journal Name:
- The Astrophysical Journal
- Volume:
- 931
- Issue:
- 1
- ISSN:
- 0004-637X
- Page Range / eLocation ID:
- 17
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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- Free Publicly Accessible Full Text
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Accepted Manuscript
- Journal Article:
- https://doi.org/10.3847/1538-4357/ac64a3
