Probing the Mass--Redshift Dependence of Binary Black Holes and its Implications for H 0 with GWTC-5.0
astro-ph.CO, astro-ph.HE
Submitted: 2026-09-22
Updated: 2026-09-22
Comments: 22 pages, 4 figures, 2 tables
License: http://creativecommons.org/licenses/by/4.0/
The gist: The mass and redshift distributions of merging binary black holes (BBHs) bear imprints of their astrophysical formation channels.
Terminology
Abstract
The mass and redshift distributions of merging binary black holes (BBHs) bear imprints of their astrophysical formation channels. Whether the BH mass distribution evolves with redshift, however, remains an open question. In this paper, we employ copula functions, which describe the dependence between variables independently of their marginal distributions, to probe the dependence structure between the primary mass and the redshift of BBH mergers. We construct five population models by coupling the marginal distributions of primary mass and redshift with the Gaussian copula, the Clayton copula, or one of its three rotations, and we constrain their hyperparameters using 235 BBH events from GWTC-5.0. For comparison, we also adopt a baseline model in which the primary mass and redshift are assumed independent. Among the copula-based models, only the model with the 180 rotated Clayton copula, which couples higher primary masses preferentially with high redshifts, exhibits evidence for a nonzero correlation, with its copula parameter deviating from the independence limit at more than 1σ significance. Importantly, the constraints on the Hubble constant (H 0) derived from these models are mutually consistent within the 68% confidence level; the baseline model yields H 0=74.3+13.7-19.6 km s-1 Mpc-1, indicating that allowing for a mass--redshift dependence does not significantly bias the H 0 inference with the current dataset. Bayesian model comparison favors the baseline model over all copula-based alternatives, with log-Bayes factors corresponding to weak to moderate evidence against the latter on the Jeffreys scale. Our results thus imply that the current GWTC-5.0 sample remains consistent with no redshift evolution of the primary mass distribution over the redshift range probed.
Sources
- Observation of Gravitational Waves from a Binary Black Hole Merger
- GWTC-5.0: Observations from the Second Part of the Fourth LIGO-Virgo-KAGRA Observing Run and Updates to the Gravitational-Wave Transient Catalog
- GW170817: Observation of Gravitational Waves from a Binary Neutron Star Inspiral
- GW190425: Observation of a Compact Binary Coalescence with Total Mass $\sim 3.4 M_{\odot}$
- Observation of gravitational waves from two neutron star-black hole coalescences
- Population Properties of Compact Objects from the Second LIGO-Virgo Gravitational-Wave Transient Catalog
- The population of merging compact binaries inferred using gravitational waves through GWTC-3
- GWTC-5.0: Population Properties of Merging Compact Binaries
- GWTC-4.0: Population Properties of Merging Compact Binaries
- Double Compact Objects III: Gravitational Wave Detection Rates
- The progenitors of compact-object binaries: impact of metallicity, common envelope and natal kicks
- Populations of stellar mass Black holes from binary systems
- The effect of the metallicity-specific star formation history on double compact object mergers
- The locations of features in the mass distribution of merging binary black holes are robust against uncertainties in the metallicity-dependent cosmic star formation history
- No peaks without valleys: The stable mass transfer channel for gravitational-wave sources in light of the neutron star-black hole mass gap
- The Effect of Pair-Instability Mass Loss on Black Hole Mergers
- Pulsational Pair-Instability Supernovae
- Very massive stars, pair-instability supernovae and intermediate-mass black holes with the SEVN code
- The impact of pair-instability mass loss on the binary black hole mass distribution
- Measuring the binary black hole mass spectrum with an astrophysically motivated parameterization
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