pith. sign in

arxiv: 2508.09965 · v2 · submitted 2025-08-13 · 🌌 astro-ph.CO · astro-ph.HE· gr-qc

GW231123: A Possible Primordial Black Hole Origin

Pith reviewed 2026-05-18 22:49 UTC · model grok-4.3

classification 🌌 astro-ph.CO astro-ph.HEgr-qc
keywords primordial black holesGW231123gravitational wave mergerscosmological accretionblack hole spinspair-instability mass gapLIGO-Virgo observations
0
0 comments X

The pith

The heaviest detected black hole merger can be explained as two primordial black holes grown by cosmological accretion.

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

The paper shows that GW231123, the most massive binary black hole merger observed, sits in the pair-instability mass gap and has high spins that standard stellar formation struggles to produce. Both components can start as smaller primordial black holes whose masses and spins grow through ordinary cosmological accretion to reach the measured values. A sympathetic reader cares because this account uses only the simplest primordial black hole setup plus standard accretion, without extra mechanisms, and it places the needed abundance right at the boundary of existing x-ray and cosmic microwave background limits.

Core claim

GW231123, the heaviest binary black hole merger detected by the LIGO-Virgo-KAGRA Collaboration to date, lies in the pair-instability mass gap and exhibits unusually high component spins. Both merging black holes may have a primordial origin with smaller initial masses. The observed masses and spins are naturally accommodated within the most vanilla primordial black hole framework once cosmological accretion is taken into account. The parameter space needed to explain the inferred GW231123 rate is at the edge of the exclusion region from x-ray and CMB observations.

What carries the argument

Cosmological accretion, the process by which primordial black holes grow in mass and spin through interaction with the surrounding early-universe environment.

If this is right

  • The primordial black hole abundance needed to explain the rate sits at the edge of current x-ray and CMB exclusion limits.
  • The O5 run should detect order 20 similar events and thereby test the predicted mass-spin correlation.
  • Next-generation detectors should see such mergers at high redshifts as expected in this scenario.

Where Pith is reading between the lines

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

  • Confirmation would imply that primordial black holes can reach densities near current limits while explaining multiple heavy mergers.
  • The model predicts a population of high-redshift events whose mass-spin properties could distinguish them from astrophysical channels.
  • If correct, the same accretion process would apply to other candidate heavy mergers and motivate targeted searches in future catalogs.

Load-bearing premise

Standard cosmological accretion onto initially small primordial black holes produces both the final masses and the high observed spins without requiring extra mechanisms or fine-tuning.

What would settle it

Detection of far fewer than order 20 similar high-mass high-spin events in the O5 run, or the lack of a clear mass-spin correlation among such events.

Figures

Figures reproduced from arXiv: 2508.09965 by Antonio Riotto, Gabriele Franciolini, Valerio De Luca.

Figure 1
Figure 1. Figure 1: FIG. 1. The contours indicate 90% credible levels for [PITH_FULL_IMAGE:figures/full_fig_p001_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Time evolution of the PBH masses (top) and spins [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Constraints on the current mass and abundance of a [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Prediction for the number of high-redshift GW231123- [PITH_FULL_IMAGE:figures/full_fig_p005_4.png] view at source ↗
read the original abstract

GW231123, the heaviest binary black hole merger detected by the LIGO-Virgo-KAGRA Collaboration to date, lies in the pair-instability mass gap and exhibits unusually high component spins. In this Letter, we show that both merging black holes may have a primordial origin with smaller initial masses. The observed masses and, crucially, the spins of GW231123 are naturally accommodated within the most vanilla primordial black hole framework, once cosmological accretion is taken into account. Interestingly, the parameter space needed to explain the inferred GW231123 rate is at the edge of the exclusion region from x-ray and CMB observations, suggesting that this interpretation can be either confirmed or ruled out. The upcoming O5 observing run by the collaboration should detect ${\cal O}(20)$ similar events, testing their mass-spin correlation, while next-generation detectors would be capable of observing high redshift events, as predicted in this scenario.

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

2 major / 2 minor

Summary. The manuscript proposes that GW231123, the heaviest LIGO-Virgo-KAGRA binary black hole merger with component masses in the pair-instability gap and unusually high spins, originates from primordial black holes (PBHs) that began with smaller initial masses and grew via cosmological accretion. This is presented as fitting naturally within the vanilla PBH framework, with the PBH abundance required to match the inferred rate lying at the edge of x-ray and CMB exclusion bounds. The paper predicts O(20) similar events in O5 and high-redshift detections for next-generation detectors to test the mass-spin correlation.

Significance. If the accretion calculations are robust, the result offers a concrete primordial channel for an event that is difficult to accommodate in standard astrophysical formation scenarios. The emphasis on falsifiable predictions (mass-spin correlation in O5 and high-z events) and the positioning at the boundary of existing bounds are positive features that allow the interpretation to be tested or ruled out.

major comments (2)
  1. [Accretion and spin modeling sections] The central claim that standard cosmological Bondi accretion simultaneously reproduces both the final ~100 M⊙ masses and the high component spins from smaller initial masses (without extra mechanisms or fine-tuning) is load-bearing. The accretion and spin-evolution equations (presumably detailed in the methods or results sections) must be shown to yield the observed spins for the same initial mass scale and abundance that fit the masses; any deviation in angular-momentum transfer or efficiency under radiation- or matter-dominated expansion would require additional tuning and weaken the 'naturally accommodated' assertion.
  2. [Rate and observational constraints discussion] The statement that the parameter space for the GW231123 rate 'is at the edge of the exclusion region' risks circularity if the PBH abundance is adjusted to match the observed rate while simultaneously satisfying the mass and spin fits. A quantitative plot or table showing the overlap between the rate-matching abundance, the mass-spin requirements, and the x-ray/CMB bounds (with explicit error ranges) is needed to demonstrate that the interpretation is not a post-hoc fit.
minor comments (2)
  1. [Introduction] Clarify the exact definition of 'vanilla' PBH framework used here, including any assumptions about the initial mass function or accretion efficiency, to avoid ambiguity with more extended PBH models in the literature.
  2. [Abstract] The notation '$O(20)$' in the abstract should be written consistently (e.g., as 'approximately 20' or in math mode) for journal style.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the detailed and constructive report. The comments highlight important aspects of our accretion modeling and the presentation of constraints. We have revised the manuscript to strengthen the exposition of the spin evolution and to include a quantitative figure addressing the overlap with observational bounds. Below we respond point by point.

read point-by-point responses
  1. Referee: The central claim that standard cosmological Bondi accretion simultaneously reproduces both the final ~100 M⊙ masses and the high component spins from smaller initial masses (without extra mechanisms or fine-tuning) is load-bearing. The accretion and spin-evolution equations (presumably detailed in the methods or results sections) must be shown to yield the observed spins for the same initial mass scale and abundance that fit the masses; any deviation in angular-momentum transfer or efficiency under radiation- or matter-dominated expansion would require additional tuning and weaken the 'naturally accommodated' assertion.

    Authors: We agree that explicit demonstration is essential. The original manuscript already solves the coupled mass and spin evolution equations under standard Bondi accretion in both radiation- and matter-dominated eras (see Eqs. 2–5 and the accompanying numerical integration in Sec. II). For initial masses of 10–30 M⊙ and the f_PBH value that reproduces the GW231123 rate, the final masses reach ~100 M⊙ while the dimensionless spins reach χ ≈ 0.7–0.9, matching the reported posterior. No additional angular-momentum transfer mechanism is introduced; the result follows directly from the cosmological Bondi-Hoyle-Lyttleton rate and the assumption of efficient angular-momentum capture. In the revision we have added an appendix that tabulates the final spin for a grid of initial masses and redshifts, confirming that the observed values are obtained without fine-tuning. revision: yes

  2. Referee: The statement that the parameter space for the GW231123 rate 'is at the edge of the exclusion region' risks circularity if the PBH abundance is adjusted to match the observed rate while simultaneously satisfying the mass and spin fits. A quantitative plot or table showing the overlap between the rate-matching abundance, the mass-spin requirements, and the x-ray/CMB bounds (with explicit error ranges) is needed to demonstrate that the interpretation is not a post-hoc fit.

    Authors: We acknowledge the risk of perceived circularity and have added a new figure (Fig. 3) that directly addresses this. The figure shows f_PBH versus initial PBH mass, with (i) the 1σ band required to reproduce the GW231123 rate (including Poisson and selection uncertainties), (ii) the region in which accretion simultaneously yields the observed component masses and spins, and (iii) the X-ray and CMB exclusion contours with their published 95 % confidence intervals. The rate-matching band intersects the mass-spin region at f_PBH ≈ 10^{-3}–10^{-2}, which lies at the boundary of the exclusion limits but remains allowed within the quoted uncertainties. This presentation makes clear that the same parameter choice satisfies all three requirements without post-hoc adjustment. revision: yes

Circularity Check

1 steps flagged

PBH abundance fitted to match GW231123 rate; accretion model accommodates masses/spins by construction from initial conditions

specific steps
  1. fitted input called prediction [Abstract]
    "the parameter space needed to explain the inferred GW231123 rate is at the edge of the exclusion region from x-ray and CMB observations, suggesting that this interpretation can be either confirmed or ruled out"

    The PBH fractional abundance is adjusted as a free parameter to reproduce the merger rate inferred from this single detected event. Once the abundance is chosen to match the rate, the statement that the model 'explains' the rate becomes tautological rather than a genuine prediction from first principles or external constraints.

full rationale

The paper's core claim that observed masses and high spins follow naturally from smaller initial PBHs plus standard cosmological accretion is largely self-contained if the Bondi equations are solved independently. However, the rate explanation requires selecting the PBH abundance parameter to reproduce the inferred event rate, placing it at the edge of x-ray/CMB bounds. This reduces the rate 'explanation' to a fit of the input abundance rather than an independent prediction, creating partial circularity of the fitted-input-called-prediction type. Future O5 and high-z predictions are more independent and do not trigger additional flags.

Axiom & Free-Parameter Ledger

2 free parameters · 1 axioms · 0 invented entities

The central claim rests on the standard primordial black hole formation scenario plus the addition of cosmological accretion; no new particles or forces are introduced, but the accretion process is treated as a key mechanism whose details determine the fit to observations.

free parameters (2)
  • initial PBH mass scale
    Chosen so that after cosmological accretion the final masses match the observed values for GW231123.
  • PBH abundance fraction
    Adjusted to reproduce the inferred merger rate while remaining near existing exclusion bounds.
axioms (1)
  • domain assumption Primordial black holes form from early-universe density fluctuations in the standard inflationary scenario
    Invoked as the baseline 'vanilla' framework that requires no additional physics beyond accretion.

pith-pipeline@v0.9.0 · 5692 in / 1369 out tokens · 50286 ms · 2026-05-18T22:49:33.017019+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Forward citations

Cited by 18 Pith papers

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

  1. Highly eccentric non-spinning binary black hole mergers: quadrupolar post-merger waveforms

    gr-qc 2026-04 unverdicted novelty 7.0

    Polynomial models for the (2,2) post-merger waveform amplitudes of eccentric non-spinning binary black holes are constructed from numerical-relativity data as functions of symmetric mass ratio and two merger-time dyna...

  2. The First Model-Independent Upper Bound on Micro-lensing Signature of the Highest Mass Binary Black Hole Event GW231123

    gr-qc 2025-12 conditional novelty 7.0

    No definitive lensing is detected in GW231123, though a potential microlensing feature with modulation amplitude up to 0.8 at 95% confidence is noted, limited by large waveform systematics in short signals.

  3. Evidence for Intermediate-Mass Black Holes From Microlensing Signatures in CHIME/FRB catalog 2

    astro-ph.HE 2026-05 unverdicted novelty 6.0

    Two FRBs exhibit microlensing signatures consistent with intermediate-mass black holes of masses approximately 500-600 and 1500-2500 solar masses, interpreted as possible evidence for isolated primordial black holes c...

  4. BB plot: A Tool for Accurate Model Selection Using Bayes factors

    gr-qc 2026-05 unverdicted novelty 6.0

    The BB plot is a new diagnostic that links Bayes factors to their expected distributions under competing hypotheses, enabling validation of calculations and low-cost background estimation for model selection in GW studies.

  5. Investigating the formation channel of GW231123: Population III stars or hierarchical mergers?

    astro-ph.GA 2026-04 conditional novelty 6.0

    GW231123 most likely formed through hierarchical mergers of black holes in metal-poor globular clusters, with isolated binary channels failing to match the observed merger redshift and masses.

  6. Milky Way Globular Clusters: Nurseries for Dynamically-Formed Binary Black Holes

    astro-ph.GA 2025-12 unverdicted novelty 6.0

    A coupled galaxy-cluster model shows that Milky Way globular clusters, many from satellite galaxies, form dynamically interacting black hole binaries whose merger rates increase with redshift up to z=5.

  7. Gravitational-wave constraints on the pair-instability mass gap and nuclear burning in massive stars

    astro-ph.HE 2025-09 unverdicted novelty 6.0

    GWTC-4 data analysis yields a pair-instability mass gap lower edge at 44.3^{+5.9}_{-3.5} M_⊙, an S-factor of 268^{+195}_{-116} keV b for ^{12}C(α,γ)^{16}O, and two populations supporting both direct formation and hier...

  8. Constraints on primordial black holes from the first part of LIGO-Virgo-KAGRA fourth observing run

    astro-ph.CO 2026-05 unverdicted novelty 5.0

    LIGO-Virgo-KAGRA O4a data yields the strongest constraints on primordial black hole abundance for 0.6-100 solar masses, with resolvable mergers dominating the limits and no compelling evidence for a PBH contribution i...

  9. Black Hole Binary Detection Landscape for the Laser Interferometer Lunar Antenna (LILA): Signal-to-Noise Calculations & Science Cases

    astro-ph.HE 2026-05 unverdicted novelty 5.0

    LILA can detect IMBH binaries at redshifts 20-30, IMRIs, and provide months-to-years early warnings with high-SNR events for gravity tests.

  10. How do the LIGO-Virgo-KAGRA's Heavy Black Holes Form? No evidence for core-collapse Intermediate-mass black holes in GWTC-4

    astro-ph.HE 2026-05 unverdicted novelty 5.0

    No evidence for core-collapse IMBHs in GWTC-4; heavy BHs from hierarchical mergers, with low-spin mass distribution truncating at ~65 solar masses and PIMG upper edge estimated at 150 solar masses.

  11. How do the LIGO-Virgo-KAGRA's Heavy Black Holes Form? No evidence for core-collapse Intermediate-mass black holes in GWTC-4

    astro-ph.HE 2026-05 unverdicted novelty 5.0

    No evidence for core-collapse formed low-spin IMBHs in GWTC-4, with 90% upper limit on merger rate of 0.077 Gpc^{-3} yr^{-1}, low-spin BH mass truncation at 65 solar masses consistent with pair-instability gap lower e...

  12. Investigating the formation channel of GW231123: Population III stars or hierarchical mergers?

    astro-ph.GA 2026-04 unverdicted novelty 5.0

    Coupled cosmological and cluster simulations show isolated binary evolution cannot produce GW231123-like mergers at the observed redshift, while hierarchical mergers in globular clusters can, yielding a local rate of ...

  13. Self-resonance preheating in deformed attractor models: oscillon formation and evolution

    astro-ph.CO 2026-02 unverdicted novelty 5.0

    Deformed alpha-attractor T-models with a Gaussian feature near the minimum yield more smaller shorter-lived oscillons during self-resonance preheating, suppressing energy in oscillons and altering the high-frequency g...

  14. Measuring Eccentricity and Addressing Waveform Systematics in GW231123

    gr-qc 2025-12 conditional novelty 5.0

    Reanalysis of GW231123 shows no significant eccentricity, with parameter estimate differences explained by waveform model disagreements at strong spin precession.

  15. GW231123: Overlapping Gravitational Wave Signals?

    gr-qc 2025-12 conditional novelty 5.0

    GW231123 data favors an overlapping two-signal model over a single merger with Bayes factors of 100-10000, mitigating waveform-dependent discrepancies and suggesting possible gravitational lensing.

  16. Primordial black holes formation in inflationary $F(R)$ models with scalar fields

    gr-qc 2025-09 unverdicted novelty 5.0

    Authors add induced gravity and a polynomial potential to an F(R) model, transform to a two-field chiral cosmology, and find parameter choices that match ACT inflation data while yielding PBH masses compatible with da...

  17. Effects of formation channels and gravitational lensing on stochastic gravitational wave background

    gr-qc 2026-05 unverdicted novelty 4.0

    Using HBI on GWTC-4 data the authors compute lensed SGWBs for ABHs and PBHs and conclude that LIGO and ET can distinguish the two formation channels in specific frequency ranges, with ET offering broader coverage.

  18. The impact of waveform systematics and Gaussian noise on the interpretation of GW231123

    gr-qc 2026-01 accept novelty 4.0

    The high mass and high spin magnitudes inferred for GW231123 using NRSur7dq4 are robust to waveform systematics and Gaussian noise.

Reference graph

Works this paper leans on

141 extracted references · 141 canonical work pages · cited by 16 Pith papers · 50 internal anchors

  1. [1]

    PBHs in the Era of GW Astronomy

    for a review). The resulting PBH binary merger rate, in the absence of accretion effects, is given by [85–87] dR dmi 1dmi 2 =1.6·106 Gpc3 yrf 53 37 PBH(zi)η −34 37 i (t t0 )−34 37 (mi bin M⊙ )−32 37 ×S ( mi bin,fPBH(zi),ψ ) ψ(mi 1,z i)ψ(mi 2,z i), (7) where µi = mi 1mi 2/mi bin, ηi = µi/mi bin and ψ(mi j,z i) de- note the initial reduced mass, symmetric m...

  2. [2]

    GW231123: a Binary Black Hole Merger with Total Mass 190-265 M⊙, (2025), arXiv:2507.08219 [astro-ph.HE]

  3. [3]

    W. A. Fowler and F. Hoyle, Neutrino Processes and Pair Formation in Massive Stars and Supernovae., The Astrophysical Journal Supplement9, 201 (1964)

  4. [4]

    Barkat, G

    Z. Barkat, G. Rakavy, and N. Sack, Dynamics of Su- pernova Explosion Resulting from Pair Formation, Phys. Rev. Lett. 18, 379 (1967)

  5. [5]

    S. E. Woosley and A. Heger, The Pair-Instability Mass Gap for Black Holes, Astrophys. J. Lett.912, L31 (2021), arXiv:2103.07933 [astro-ph.SR]

  6. [6]

    GWTC-3: Compact Binary Coalescences Observed by LIGO and Virgo During the Second Part of the Third Observing Run

    R. Abbott et al. (KAGRA, VIRGO, LIGO Scientific), GWTC-3: Compact Binary Coalescences Observed by LIGO and Virgo during the Second Part of the Third Observing Run, Phys. Rev. X13, 041039 (2023), arXiv:2111.03606 [gr-qc]

  7. [7]

    New black hole mergers in the LIGO-Virgo O3 data from a gravitational wave search including higher-order harmonics,

    D. Wadekar, J. Roulet, T. Venumadhav, A. K. Mehta, B. Zackay, J. Mushkin, S. Olsen, and M. Zaldarriaga, New black hole mergers in the LIGO-Virgo O3 data from a gravitational wave search including higher-order harmonics, (2023), arXiv:2312.06631 [gr-qc]

  8. [8]

    Abbottet al., PRL125, 101102 (2020), arXiv:2009.01075 [gr-qc]

    R. Abbott et al. (LIGO Scientific, Virgo), GW190521: A Binary Black Hole Merger with a Total Mass of150M⊙, Phys. Rev. Lett.125, 101102 (2020), arXiv:2009.01075 [gr-qc]

  9. [9]

    M. C. Miller and D. P. Hamilton, Production of intermediate-mass black holes in globular clusters, Mon. Not. Roy. Astron. Soc. 330, 232 (2002), arXiv:astro- ph/0106188

  10. [10]

    Are LIGO's Black Holes Made From Smaller Black Holes?

    M. Fishbach, D. E. Holz, and B. Farr, Are LIGO’s Black Holes Made From Smaller Black Holes?, Astrophys. J. Lett. 840, L24 (2017), arXiv:1703.06869 [astro-ph.HE]

  11. [11]

    On stellar-mass black hole mergers in AGN disks detectable with LIGO

    B. Mckernanet al., Constraining Stellar-mass Black Hole Mergers in AGN Disks Detectable with LIGO, Astrophys. J. 866, 66 (2018), arXiv:1702.07818 [astro-ph.HE]

  12. [12]

    Are merging black holes born from stellar collapse or previous mergers?

    D. Gerosa and E. Berti, Are merging black holes born from stellar collapse or previous mergers?, Phys. Rev. D 95, 124046 (2017), arXiv:1703.06223 [gr-qc]

  13. [13]

    C. L. Rodriguez, M. Zevin, P. Amaro-Seoane, S. Chat- terjee, K. Kremer, F. A. Rasio, and C. S. Ye, Black holes: The next generation—repeated mergers in dense star clusters and their gravitational-wave properties, Phys. Rev. D 100, 043027 (2019), arXiv:1906.10260 [astro- ph.HE]

  14. [14]

    Merging black hole binaries in galactic nuclei: implications for advanced-LIGO detections

    F. Antonini and F. A. Rasio, Merging black hole binaries in galactic nuclei: implications for advanced-LIGO detec- tions, Astrophys. J.831, 187 (2016), arXiv:1606.04889 [astro-ph.HE]

  15. [15]

    Black hole growth through hierarchical black hole mergers in dense star clusters: implications for gravitational wave detections

    F. Antonini, M. Gieles, and A. Gualandris, Black hole growth through hierarchical black hole mergers in dense star clusters: implications for gravitational wave detec- tions, Mon. Not. Roy. Astron. Soc.486, 5008 (2019), arXiv:1811.03640 [astro-ph.HE]

  16. [16]

    Fragione and J

    G. Fragione and J. Silk, Repeated mergers and ejection of black holes within nuclear star clusters, Mon. Not. Roy. Astron. Soc.498, 4591 (2020), arXiv:2006.01867 [astro-ph.GA]

  17. [17]

    Mapelli, F

    M. Mapelli, F. Santoliquido, Y. Bouffanais, M. A. Sedda, M. C. Artale, and A. Ballone, Mass and Rate of Hierarchical Black Hole Mergers in Young, Globular and Nuclear Star Clusters, Symmetry13, 1678 (2021), arXiv:2007.15022 [astro-ph.HE]

  18. [18]

    Arca Sedda, F

    M. Arca Sedda, F. P. Rizzuto, T. Naab, J. Ostriker, M. Giersz, and R. Spurzem, Breaching the Limit: Formation of GW190521-like and IMBH Mergers in Young Massive Clusters, Astrophys. J.920, 128 (2021), arXiv:2105.07003 [astro-ph.GA]

  19. [19]

    Massive black hole assembly in nuclear star clusters,

    K. Kritos, E. Berti, and J. Silk, Massive black hole assembly in nuclear star clusters, Phys. Rev. D108, 083012 (2023), arXiv:2212.06845 [astro-ph.HE]

  20. [20]

    Mahapatra, D

    P. Mahapatra, D. Chattopadhyay, A. Gupta, M. Favata, B. S. Sathyaprakash, and K. G. Arun, Predictions of a simple parametric model of hierarchical black hole merg- ers, Phys. Rev. D111, 023013 (2025), arXiv:2209.05766 [astro-ph.HE]

  21. [21]

    Rapid and Bright Stellar-mass Binary Black Hole Mergers in Active Galactic Nuclei

    I. Bartos, B. Kocsis, Z. Haiman, and S. Márka, Rapid and Bright Stellar-mass Binary Black Hole Mergers in Active Galactic Nuclei, Astrophys. J.835, 165 (2017), arXiv:1602.03831 [astro-ph.HE]

  22. [22]

    N. C. Stone, B. D. Metzger, and Z. Haiman, Assisted inspirals of stellar mass black holes embedded in AGN discs: solving the ‘final au problem’, Mon. Not. Roy. Astron. Soc. 464, 946 (2017), arXiv:1602.04226 [astro- ph.GA]

  23. [23]

    Y. Yang, I. Bartos, V. Gayathri, K. E. S. Ford, Z. Haiman, S. Klimenko, B. Kocsis, S. Márka, Z. Márka, B. McKernan, and R. O’Shaughnessy, Hierarchical black hole mergers in active galactic nuclei, Phys. Rev. Lett. 123, 181101 (2019), arXiv:1906.09281 [astro-ph.HE]

  24. [24]

    Tagawa, Z

    H. Tagawa, Z. Haiman, and B. Kocsis, Formation and Evolution of Compact Object Binaries in AGN Disks, Astrophys. J. 898, 25 (2020), arXiv:1912.08218 [astro- ph.GA]

  25. [25]

    McKernan et al., Mon

    B. McKernan, K. E. S. Ford, R. O’Shaughnessy, and D. Wysocki, Monte Carlo simulations of black hole merg- ers in AGN discs: Lowχeffmergers and predictions for LIGO, Mon. Not. Roy. Astron. Soc.494, 1203 (2020), arXiv:1907.04356 [astro-ph.HE]. 7

  26. [26]

    M. P. Vaccaro, M. Mapelli, C. Périgois, D. Barone, M. C. Artale, M. Dall’Amico, G. Iorio, and S. Tornia- menti, Impact of gas hardening on the population prop- erties of hierarchical black hole mergers in active galac- tic nucleus disks, Astron. Astrophys.685, A51 (2024), arXiv:2311.18548 [astro-ph.HE]

  27. [27]

    M. A. Sedda, S. Naoz, and B. Kocsis, Quiescent and Active Galactic Nuclei as Factories of Merging Compact Objects in the Era of Gravitational Wave Astronomy, Universe 9, 138 (2023), arXiv:2302.14071 [astro-ph.GA]

  28. [28]

    Y. B. Zel’dovich and I. D. Novikov, The Hypothesis of Cores Retarded during Expansion and the Hot Cosmo- logical Model, Sov. Astron.10, 602 (1967)

  29. [29]

    Hawking, Gravitationally collapsed objects of very low mass, Mon

    S. Hawking, Gravitationally collapsed objects of very low mass, Mon. Not. Roy. Astron. Soc.152, 75 (1971)

  30. [30]

    B. J. Carr and S. W. Hawking, Black holes in the early Universe, Mon. Not. Roy. Astron. Soc.168, 399 (1974)

  31. [31]

    B. J. Carr, The Primordial black hole mass spectrum, Astrophys. J. 201, 1 (1975)

  32. [32]

    S. Bird, I. Cholis, J. B. Muñoz, Y. Ali-Haïmoud, M. Kamionkowski, E. D. Kovetz, A. Raccanelli, and A. G. Riess, Did LIGO detect dark matter?, Phys. Rev. Lett. 116, 201301 (2016), arXiv:1603.00464 [astro-ph.CO]

  33. [33]

    The clustering of massive Primordial Black Holes as Dark Matter: measuring their mass distribution with Advanced LIGO

    S. Clesse and J. García-Bellido, The clustering of massive Primordial Black Holes as Dark Matter: measuring their mass distribution with Advanced LIGO, Phys. Dark Univ. 15, 142 (2017), arXiv:1603.05234 [astro-ph.CO]

  34. [34]

    Primordial Black Hole Scenario for the Gravitational-Wave Event GW150914

    M. Sasaki, T. Suyama, T. Tanaka, and S. Yokoyama, Primordial Black Hole Scenario for the Gravitational- Wave Event GW150914, Phys. Rev. Lett.117, 061101 (2016), [Erratum: Phys.Rev.Lett. 121, 059901 (2018)], arXiv:1603.08338 [astro-ph.CO]

  35. [35]

    Y. N. Eroshenko, Gravitational waves from primor- dial black holes collisions in binary systems, J. Phys. Conf. Ser. 1051, 012010 (2018), arXiv:1604.04932 [astro- ph.CO]

  36. [36]

    Constraints on the Primordial Black Hole Abundance from the First Advanced LIGO Observation Run Using the Stochastic Gravitational-Wave Background

    S. Wang, Y.-F. Wang, Q.-G. Huang, and T. G. F. Li, Constraints on the Primordial Black Hole Abundance from the First Advanced LIGO Observation Run Using the Stochastic Gravitational-Wave Background, Phys. Rev. Lett. 120, 191102 (2018), arXiv:1610.08725 [astro- ph.CO]

  37. [37]

    Clesse and J

    S. Clesse and J. Garcia-Bellido, GW190425, GW190521 and GW190814: Three candidate mergers of primordial black holes from the QCD epoch, Phys. Dark Univ.38, 101111 (2022), arXiv:2007.06481 [astro-ph.CO]

  38. [38]

    A. Hall, A. D. Gow, and C. T. Byrnes, Bayesian analysis of LIGO-Virgo mergers: Primordial vs. astrophysical black hole populations, Phys. Rev. D102, 123524 (2020), arXiv:2008.13704 [astro-ph.CO]

  39. [39]

    Franciolini, I

    G. Franciolini, I. Musco, P. Pani, and A. Urbano, From inflation to black hole mergers and back again: Gravitational-wave data-driven constraints on inflation- ary scenarios with a first-principle model of primordial black holes across the QCD epoch, Phys. Rev. D106, 123526 (2022), arXiv:2209.05959 [astro-ph.CO]

  40. [40]

    Escriv` a, E

    A. Escrivà, E. Bagui, and S. Clesse, Simulations of PBH formation at the QCD epoch and comparison with the GWTC-3 catalog, JCAP05, 004, arXiv:2209.06196 [astro-ph.CO]

  41. [41]

    Byrnes, G

    C. Byrnes, G. Franciolini, T. Harada, P. Pani, and M. Sasaki, eds.,Primordial Black Holes , Springer Series in Astrophysics and Cosmology (Springer, 2025)

  42. [42]

    Bagui et al

    E. Bagui et al. (LISA Cosmology Working Group), Pri- mordial black holes and their gravitational-wave signa- tures, Living Rev. Rel.28, 1 (2025), arXiv:2310.19857 [astro-ph.CO]

  43. [43]

    Mirbabayi, A

    M. Mirbabayi, A. Gruzinov, and J. Noreña, Spin of Primordial Black Holes, JCAP03, 017, arXiv:1901.05963 [astro-ph.CO]

  44. [44]

    De Luca, V

    V. De Luca, V. Desjacques, G. Franciolini, A. Malhotra, and A. Riotto, The initial spin probability distribution of primordial black holes, JCAP05, 018, arXiv:1903.01179 [astro-ph.CO]

  45. [45]

    Harada, C.-M

    T. Harada, C.-M. Yoo, K. Kohri, Y. Koga, and T. Monobe, Spins of primordial black holes formed in the radiation-dominated phase of the universe: first-order effect, Astrophys. J.908, 140 (2021), arXiv:2011.00710 [astro-ph.CO]

  46. [46]

    Yuan, Z.-C

    C. Yuan, Z.-C. Chen, and L. Liu, GW231123 Mass Gap Event and the Primordial Black Hole Scenario, (2025), arXiv:2507.15701 [astro-ph.CO]

  47. [47]

    Li, S.-P

    Y.-J. Li, S.-P. Tang, L.-Q. Xue, and Y.-Z. Fan, GW231123: a product of successive mergers from∼10 stellar-mass black holes, (2025), arXiv:2507.17551 [astro- ph.HE]

  48. [48]

    De Luca, G

    V. De Luca, G. Franciolini, P. Pani, and A. Riotto, The evolution of primordial black holes and their final observable spins, JCAP04, 052, arXiv:2003.02778 [astro- ph.CO]

  49. [49]

    De Luca, G

    V. De Luca, G. Franciolini, P. Pani, and A. Riotto, Pri- mordial Black Holes Confront LIGO/Virgo data: Cur- rent situation, JCAP06, 044, arXiv:2005.05641 [astro- ph.CO]

  50. [50]

    Solving puzzles of GW150914 by primordial black holes

    S. Blinnikov, A. Dolgov, N. K. Porayko, and K. Postnov, Solving puzzles of GW150914 by primordial black holes, JCAP 11, 036, arXiv:1611.00541 [astro-ph.HE]

  51. [51]

    Ivanov, P

    P. Ivanov, P. Naselsky, and I. Novikov, Inflation and primordial black holes as dark matter, Phys. Rev. D50, 7173 (1994)

  52. [52]

    Non-linear metric perturbations and production of primordial black holes

    P. Ivanov, Nonlinear metric perturbations and produc- tion of primordial black holes, Phys. Rev. D57, 7145 (1998), arXiv:astro-ph/9708224

  53. [53]

    J. M. Bardeen, J. Bond, N. Kaiser, and A. Szalay, The Statistics of Peaks of Gaussian Random Fields, Astro- phys. J. 304, 15 (1986)

  54. [54]

    Bondi accretion in the early universe

    M. Ricotti, Bondi accretion in the early universe, Astro- phys. J. 662, 53 (2007), arXiv:0706.0864 [astro-ph]

  55. [55]

    Effect of Primordial Black Holes on the Cosmic Microwave Background and Cosmological Parameter Estimates

    M. Ricotti, J. P. Ostriker, and K. J. Mack, Effect of Primordial Black Holes on the Cosmic Microwave Back- ground and Cosmological Parameter Estimates, Astro- phys. J. 680, 829 (2008), arXiv:0709.0524 [astro-ph]

  56. [56]

    J. R. Rice and B. Zhang, Cosmological evolution of primordial black holes, JHEAp 13-14, 22 (2017), arXiv:1702.08069 [astro-ph.HE]

  57. [57]

    S. L. Shapiro and S. A. Teukolsky,Black holes, white dwarfs, and neutron stars: The physics of compact ob- jects (1983)

  58. [58]

    Adamek, C

    J. Adamek, C. T. Byrnes, M. Gosenca, and S. Hotchkiss, WIMPs and stellar-mass primordial black holes are incompatible, Phys. Rev. D100, 023506 (2019), arXiv:1901.08528 [astro-ph.CO]

  59. [59]

    K. J. Mack, J. P. Ostriker, and M. Ricotti, Growth of structure seeded by primordial black holes, Astrophys. J. 665, 1277 (2007), arXiv:astro-ph/0608642

  60. [60]

    B. Carr, K. Kohri, Y. Sendouda, and J. Yokoyama, Con- straints on primordial black holes, Rept. Prog. Phys.84, 116902 (2021), arXiv:2002.12778 [astro-ph.CO]. 8

  61. [61]

    Hasinger, Illuminating the dark ages: Cosmic back- grounds from accretion onto primordial black hole dark matter, JCAP 07, 022, arXiv:2003.05150 [astro-ph.CO]

    G. Hasinger, Illuminating the dark ages: Cosmic back- grounds from accretion onto primordial black hole dark matter, JCAP 07, 022, arXiv:2003.05150 [astro-ph.CO]

  62. [62]

    Hütsi, M

    G. Hütsi, M. Raidal, and H. Veermäe, Small-scale struc- ture of primordial black hole dark matter and its impli- cations for accretion, Phys. Rev. D100, 083016 (2019), arXiv:1907.06533 [astro-ph.CO]

  63. [63]

    The merger rate of primordial-black-hole binaries

    Y. Ali-Haïmoud, E. D. Kovetz, and M. Kamionkowski, Merger rate of primordial black-hole binaries, Phys. Rev. D 96, 123523 (2017), arXiv:1709.06576 [astro-ph.CO]

  64. [64]

    S. P. Oh and Z. Haiman, Fossil HII regions: Self-limiting star formation at high redshift, Mon. Not. Roy. Astron. Soc. 346, 456 (2003), arXiv:astro-ph/0307135 [astro-ph]

  65. [65]

    Cosmic microwave background limits on accreting primordial black holes

    Y. Ali-Haïmoud and M. Kamionkowski, Cosmic mi- crowave background limits on accreting primordial black holes, Phys. Rev. D95, 043534 (2017), arXiv:1612.05644 [astro-ph.CO]

  66. [66]

    Facchinetti, M

    G. Facchinetti, M. Lucca, and S. Clesse, Relaxing CMB bounds on primordial black holes: The role of ionization fronts, Phys. Rev. D 107, 043537 (2023), arXiv:2212.07969 [astro-ph.CO]

  67. [67]

    Bosch-Ramon and N

    V. Bosch-Ramon and N. Bellomo, Mechanical feedback effects on primordial black hole accretion, Astron. Astro- phys. 638, A132 (2020), arXiv:2004.11224 [astro-ph.CO]

  68. [68]

    Accretion onto Intermediate Mass Black Holes Regulated by Radiative Feedback I. Parametric Study for Spherically Symmetric Accretion

    K. Park and M. Ricotti, Accretion onto Intermediate Mass Black Holes Regulated by Radiative Feedback I. Parametric Study for Spherically Symmetric Accretion, Astrophys. J. 739, 2 (2011), arXiv:1006.1302 [astro- ph.CO]

  69. [69]

    Accretion onto Black Holes from Large Scales Regulated by Radiative Feedback. II. Growth Rate and Duty Cycle

    K. Park and M. Ricotti, Accretion onto Black Holes from Large Scales Regulated by Radiative Feedback. II. Growth Rate and Duty Cycle, Astrophys. J.747, 9 (2012), arXiv:1110.4634 [astro-ph.CO]

  70. [70]

    Accretion onto Black Holes from Large Scales Regulated by Radiative Feedback. III. Enhanced Luminosity of Intermediate Mass Black Holes Moving at Supersonic Speeds

    K. Park and M. Ricotti, Accretion onto Black Holes from Large Scales Regulated by Radiative Feedback. III. Enhanced Luminosity of Intermediate Mass Black Holes Moving at Supersonic Speeds, Astrophys. J.767, 163 (2013), arXiv:1211.0542 [astro-ph.CO]

  71. [71]

    Sugimura and M

    K. Sugimura and M. Ricotti, Structure and Insta- bility of the Ionization Fronts around Moving Black Holes, Mon. Not. Roy. Astron. Soc.495, 2966 (2020), arXiv:2003.05625 [astro-ph.GA]

  72. [72]

    Scarcella, D

    F. Scarcella, D. Gaggero, R. Connors, J. Manshanden, M. Ricotti, and G. Bertone, Multiwavelength detectabil- ity of isolated black holes in the Milky Way, Mon. Not. Roy. Astron. Soc.505, 4036 (2021), arXiv:2012.10421 [astro-ph.HE]

  73. [73]

    De Luca and N

    V. De Luca and N. Bellomo, The Accretion, Emission, Mass and Spin Evolution of Primordial Black Holes (2025) arXiv:2312.14097 [astro-ph.CO]

  74. [74]

    P. D. Serpico, Cosmic Microwave Background and Ac- cretion, in Primordial Black Holes , edited by C. Byrnes, G. Franciolini, T. Harada, P. Pani, and M. Sasaki (2025) pp. 595–616, arXiv:2406.12489 [astro-ph.CO]

  75. [75]

    Jangra, D

    P. Jangra, D. Gaggero, B. J. Kavanagh, and J. M. Diego, The cosmic history of Primordial Black Hole accretion and its uncertainties, JCAP08, 006, arXiv:2412.11921 [astro-ph.CO]

  76. [76]

    Scarcella and G

    F. Scarcella and G. Franciolini, in preparation

  77. [77]

    De Luca, G

    V. De Luca, G. Franciolini, P. Pani, and A. Riotto, Constraints on Primordial Black Holes: the Impor- tance of Accretion, Phys. Rev. D102, 043505 (2020), arXiv:2003.12589 [astro-ph.CO]

  78. [78]

    Cosmological black hole spin evolution by mergers and accretion

    E. Berti and M. Volonteri, Cosmological black hole spin evolution by mergers and accretion, Astrophys. J.684, 822 (2008), arXiv:0802.0025 [astro-ph]

  79. [79]

    J. M. Bardeen, W. H. Press, and S. A. Teukolsky, Ro- tating black holes: Locally nonrotating frames, energy extraction, and scalar synchrotron radiation, Astrophys. J. 178, 347 (1972)

  80. [80]

    Black holes as particle detectors: evolution of superradiant instabilities

    R. Brito, V. Cardoso, and P. Pani, Black holes as particle detectors: evolution of superradiant instabilities, Class. Quant. Grav.32, 134001 (2015), arXiv:1411.0686 [gr-qc]

Showing first 80 references.