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arxiv: 2507.23663 · v2 · submitted 2025-07-31 · 🌀 gr-qc · astro-ph.HE

Disentangling spinning and nonspinning binary black hole populations with spin sorting

Pith reviewed 2026-05-19 02:19 UTC · model grok-4.3

classification 🌀 gr-qc astro-ph.HE
keywords binary black holesgravitational wavesspin sortingpopulation inferencenonspinning black holesLIGO-Virgo-KAGRAcomponent spins
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The pith

Gravitational-wave data rule out a fully nonspinning binary black hole population but allow up to 80 percent nonspinning systems.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper tests whether sorting the two black holes in each binary by spin magnitude rather than mass lets the standard population model separate spinning and nonspinning sources even when that model cannot handle an excess of zero-spin objects. Simulations of different populations show that this spin-sorting approach recovers the input spin properties reliably enough to compare with real observations. The analysis finds that existing data disagree with every black hole having zero spin. The same data stay consistent with a population in which only one component spins in each pair or with a population containing as many as 80 percent nonspinning systems.

Core claim

By coupling the Default spin magnitude population model with spin sorting on simulated binary black hole populations, spinning and nonspinning populations can be reliably distinguished despite the model's inability to formally accommodate an excess of zero-spin systems. Current observations of the BBH population are inconsistent with a fully nonspinning population but could be explained by a population with only one spinning black hole per binary or a population with up to 80 percent nonspinning sources.

What carries the argument

Spin sorting, the reordering of binary components by spin magnitude instead of mass, which reveals asymmetric spin distributions expected from tidal spin-up and other binary evolution processes.

If this is right

  • Mass-based sorting alone can miss spin asymmetries produced by tidal spin-up during binary evolution.
  • A population with only one spinning black hole per binary remains compatible with existing data.
  • Fractions of nonspinning systems as high as 80 percent are still allowed under the tested model.
  • Spin-sorting analyses can be applied to future catalogs to tighten constraints on the fraction of nonspinning sources.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The method could help isolate formation channels that naturally produce one rapidly spinning and one slowly spinning black hole.
  • Improved spin measurements in the next observing runs would allow tighter upper limits on the allowed fraction of nonspinning systems.
  • Extending spin sorting to alternative population models might expose additional signatures of spin alignment or misalignment.

Load-bearing premise

The Default spin magnitude population model remains reliable for distinguishing spinning and nonspinning populations when paired with spin sorting on simulated data, even though it cannot formally accommodate an excess of zero-spin systems.

What would settle it

A catalog containing many additional detections in which both black holes in each pair show spin magnitudes consistent with exactly zero would test whether the current exclusion of a fully nonspinning population holds.

Figures

Figures reproduced from arXiv: 2507.23663 by Lillie Szemraj, Sylvia Biscoveanu.

Figure 1
Figure 1. Figure 1: PPDs for χA (blue, left), χB (green, middle) and χ1/2 (yellow, right) inferred by the LVK for the GWTC-3 BBH population fit with a Beta distribution (the Default model), shown in the solid lines. The shaded regions correspond to the 90% credible intervals. Figure adapted from Figs. 15, 17 of [33]. when allowing for singular Beta distributions in the hyper-parameter prior (bottom panel) are much more strong… view at source ↗
Figure 2
Figure 2. Figure 2: Solid lines show the PPDs for χA (blue, left), χB (green, middle) and χ1/2 (yellow, right) inferred for the nonspinning BBH population when limiting the hyper-parameter prior to nonsingular Beta distributions (top) and including singular Beta distributions (bottom). The shaded regions (dotted lines) correspond to the 90% credible intervals for the posteriors (priors), and the magenta lines show the true di… view at source ↗
Figure 3
Figure 3. Figure 3: Posteriors on the hyper-parameters αχ, βχ for the nonspinning (spinning) population in purple (red). The solid lines show the results obtained using the priors including singular Beta distributions, and the dotted lines show the nonsingular results [PITH_FULL_IMAGE:figures/full_fig_p009_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Same as [PITH_FULL_IMAGE:figures/full_fig_p010_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Solid lines show the PPDs for χA (blue, left), χB (green, middle) and χ1/2 (yellow, right) inferred for the nonspinning (top) and singly-spinning (bottom) BBH populations analyzed using a Truncated Gaussian population model. The shaded regions (dotted lines) correspond to the 90% credible intervals for the posteriors (priors), and the magenta lines show the true distributions. both populations, the posteri… view at source ↗
Figure 6
Figure 6. Figure 6: PPDs for χA (left) and χB (right) for eleven different simulated populations with a varying fraction of nonspinning events, ranging from all nonspinning to all spinning. The top (bottom) row shows the results obtained when singular Beta distributions are excluded (included) in the prior. events each with mixture fractions evenly distributed in fnospin ∈ [0, 1] by combining our simulated nonspinning and ful… view at source ↗
Figure 7
Figure 7. Figure 7: 99th percentile of the inferred χA distributions (left) and 1st percentile of the inferred χB distributions as a function of the fraction of events in the population that are nonspinning. The shaded region bounds the 90% posterior credible interval, and the black markers show the true values for each mixed population. The results obtained when including (excluding) singular Beta distributions in the prior … view at source ↗
read the original abstract

The individual component spins of binary black holes (BBHs) are difficult to resolve using gravitational-wave observations but carry key signatures of the processes shaping their formation and evolution. Recent analyses have found conflicting evidence for a sub-population of black holes with negligible spin, but the Default spin magnitude population model used in LIGO-Virgo-KAGRA analyses cannot formally accommodate an excess of systems with zero spin. In this work, we analyze several different simulated BBH populations to demonstrate that even in the face of this mismodeling, spinning and nonspinning populations can be reliably distinguished using the Default spin magnitude population model coupled with spin sorting. While typical analyses sort the binary components by their masses, sorting the components by their spin magnitudes instead offers a complementary view of the properties of individual systems consistent with equal mass and of population-level properties, given binary evolution processes like tidal-spin up that predict asymmetric spin magnitudes among the binary components. We conclude that current observations of the BBH population are inconsistent with a fully nonspinning population, but could be explained by a population with only one spinning black hole per binary or a population with up to 80% nonspinning sources.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 2 minor

Summary. The paper analyzes multiple simulated BBH populations to demonstrate that sorting binary components by spin magnitude (rather than mass) enables the Default spin magnitude population model to distinguish spinning from nonspinning subpopulations, even though the model cannot formally place mass at exactly zero spin. Forward simulations are compared to real LVK observations, leading to the conclusion that current data are inconsistent with a fully nonspinning population but remain compatible with a population having only one spinning black hole per binary or up to 80% nonspinning sources.

Significance. If the central distinction holds under the tested conditions, the work provides a practical complementary inference method that mitigates the impact of spin-magnitude mismodeling in existing LVK population analyses. The use of several simulated populations and the explicit comparison to real-data conclusions are strengths that support falsifiability of the subpopulation claims.

major comments (1)
  1. [Simulation validation section] Simulation validation section: The load-bearing claim that spin sorting yields distinguishable posteriors on spinning vs. nonspinning fractions rests on the assumption that the injected simulated populations reproduce the precise form of model mismatch (excess systems at chi=0) that arises when the Default model is applied to real LVK data. If the simulated distributions remain closer to the Default parametric family than a true zero-spin subpopulation would be, the validation does not fully establish robustness for the observational conclusion.
minor comments (2)
  1. [Abstract] Abstract: The central claims would be easier to verify if quantitative measures such as posterior odds, credible intervals on the nonspinning fraction, or explicit simulation parameters were reported rather than qualitative statements alone.
  2. Notation: Clarify whether 'spin sorting' refers to sorting by the magnitude of the primary or secondary component after the fact or to a joint population model; the distinction affects how the results map to binary evolution predictions such as tidal spin-up.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading of our manuscript and for providing constructive feedback. We address the major comment in detail below. We have made revisions to clarify and strengthen the simulation validation section as suggested.

read point-by-point responses
  1. Referee: The load-bearing claim that spin sorting yields distinguishable posteriors on spinning vs. nonspinning fractions rests on the assumption that the injected simulated populations reproduce the precise form of model mismatch (excess systems at chi=0) that arises when the Default model is applied to real LVK data. If the simulated distributions remain closer to the Default parametric family than a true zero-spin subpopulation would be, the validation does not fully establish robustness for the observational conclusion.

    Authors: We appreciate the referee pointing out this important consideration for the robustness of our validation. Our simulations are constructed by injecting populations with varying fractions of nonspinning black holes (including up to 100% nonspinning in some cases) into the Default spin magnitude model framework. The model mismatch, characterized by an excess of systems with chi approximately 0, arises naturally in these simulations because the Default model has difficulty accommodating exact zero spins, similar to its application to real data. We have examined the recovered posteriors and confirmed that the degree of mismatch is comparable, as evidenced by the distinguishable fractions of spinning and nonspinning components when using spin sorting. To address this concern more explicitly, we will add a new figure or subsection in the simulation validation section that directly compares the chi=0 excess in the simulated posteriors to that observed in the LVK data analysis. This will further demonstrate that our simulations capture the relevant mismodeling effects. revision: yes

Circularity Check

0 steps flagged

No circularity: conclusions rest on external data and forward simulations

full rationale

The paper validates the Default spin magnitude model plus spin sorting by injecting and recovering several simulated BBH populations, then applies the same pipeline to real LVK observations. No step equates a claimed prediction or population inference to a fitted parameter or self-citation by algebraic construction; the simulation tests are independent checks against the model's known inability to place mass at exactly zero spin. The observational conclusions therefore remain externally anchored rather than self-referential.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The work rests on the standard assumptions of LIGO-Virgo-KAGRA population inference and on the fidelity of the simulated binary populations used to test the sorting procedure.

axioms (1)
  • domain assumption The Default spin magnitude population model remains usable for population distinction even though it cannot formally accommodate an excess of systems with zero spin.
    Explicitly stated in the abstract as the model employed in current LIGO analyses.

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Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. GWTC-4.0: Population Properties of Merging Compact Binaries

    astro-ph.HE 2025-08 unverdicted novelty 5.0

    Pith review generated a malformed one-line summary.

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