Supermassive black hole formation in the initial collapse of axion dark matter
Pith reviewed 2026-05-23 22:37 UTC · model grok-4.3
The pith
Axion dark matter forms supermassive black holes during the collapse of early overdensities by transporting angular momentum outward through rethermalization.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Axion dark matter thermalizes by gravitational self-interactions and forms a Bose-Einstein condensate. The rethermalization of the axion fluid during the initial collapse of large scale overdensities near cosmic dawn transports angular momentum outward sufficiently fast that black holes form with masses ranging from approximately 10^5 to a few times 10^{10} M_⊙. This conclusion holds for QCD axions and for axion-like particles of mass larger than 10^{-16} eV/c^2.
What carries the argument
Rethermalization of the axion Bose-Einstein condensate during gravitational collapse of overdensities, which carries angular momentum outward on the collapse timescale.
Load-bearing premise
Gravitational self-interactions cause axion dark matter to thermalize into a Bose-Einstein condensate whose rethermalization during collapse removes angular momentum on the timescale of the initial overdensity collapse.
What would settle it
A simulation or calculation showing that rethermalization fails to transport angular momentum outward fast enough to permit black hole formation within the collapse time of the overdensity would falsify the claim.
Figures
read the original abstract
Axion dark matter thermalizes by gravitational self-interactions and forms a Bose-Einstein condensate. We show that the rethermalization of the axion fluid during the initial collapse of large scale overdensities near cosmic dawn transports angular momentum outward sufficientlly fast that black holes form with masses ranging from approximately $10^5$ to a few times $10^{10}~M_\odot$. This conclusion holds for QCD axions and for axion-like particles of mass larger than $10^{-16}$ eV/$c^2$.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript claims that axion dark matter thermalizes via gravitational self-interactions to form a Bose-Einstein condensate, and that rethermalization during the initial collapse of large-scale overdensities near cosmic dawn transports angular momentum outward sufficiently rapidly to produce black holes with masses from ~10^5 to a few ×10^{10} M_⊙. The result is asserted to apply to QCD axions and to axion-like particles with m_a ≳ 10^{-16} eV/c².
Significance. If the central claim is substantiated by explicit timescale comparisons, the work would supply a direct-collapse channel for supermassive black holes seeded by axion overdensities, offering a potential explanation for high-redshift quasars that does not rely on stellar-mass seeds or sustained super-Eddington accretion. It would also furnish a new observable link between axion mass and the high-z black-hole mass function.
major comments (2)
- [Abstract] Abstract: the central claim that rethermalization transports angular momentum outward on the collapse timescale is stated without any derivation, numerical estimate, or comparison of τ_rel to t_collapse; the manuscript must supply this comparison (including Hubble expansion and the linear-to-nonlinear transition) to establish that the inequality holds across the quoted mass window.
- [Derivation of relaxation rate] Section deriving the relaxation rate: the gravitational scattering rate for the condensate must be shown to satisfy τ_rel ≪ t_collapse at the relevant densities, velocities, and redshifts; without an explicit evaluation that accounts for the inhomogeneous density profile during collapse, the transport efficiency remains unverified and the mass range 10^5–10^{10} M_⊙ cannot be justified.
minor comments (1)
- [Abstract] Abstract, line 3: 'sufficientlly' is a typographical error and should read 'sufficiently'.
Simulated Author's Rebuttal
We thank the referee for their careful reading and constructive comments, which help clarify the presentation of our results on axion dark matter collapse and black hole formation. We address each major comment below.
read point-by-point responses
-
Referee: [Abstract] Abstract: the central claim that rethermalization transports angular momentum outward on the collapse timescale is stated without any derivation, numerical estimate, or comparison of τ_rel to t_collapse; the manuscript must supply this comparison (including Hubble expansion and the linear-to-nonlinear transition) to establish that the inequality holds across the quoted mass window.
Authors: We agree that the abstract and main text would benefit from an explicit, consolidated comparison of τ_rel and t_collapse. The manuscript derives the relaxation rate in Section 3 and estimates collapse times near cosmic dawn, but does not tabulate the ratio including Hubble expansion and the linear-to-nonlinear transition for the full mass window. In the revision we will add this comparison (with a new figure) to Section 3 and update the abstract to reference it, confirming the inequality for m_a ≳ 10^{-16} eV/c². revision: yes
-
Referee: [Derivation of relaxation rate] Section deriving the relaxation rate: the gravitational scattering rate for the condensate must be shown to satisfy τ_rel ≪ t_collapse at the relevant densities, velocities, and redshifts; without an explicit evaluation that accounts for the inhomogeneous density profile during collapse, the transport efficiency remains unverified and the mass range 10^5–10^{10} M_⊙ cannot be justified.
Authors: We concur that an evaluation using the inhomogeneous density profile is required to rigorously justify the mass range. The present derivation employs a mean-density approximation for the gravitational scattering rate. The revised manuscript will add an appendix containing explicit calculations of τ_rel at multiple points along the collapse trajectory (using the spherical-collapse density profile), evaluated at the relevant redshifts, velocities, and axion masses. These will demonstrate that τ_rel ≪ t_collapse holds across the quoted window. revision: yes
Circularity Check
No significant circularity detected; derivation treated as self-contained.
full rationale
No load-bearing steps could be identified that reduce by the paper's own equations or self-citation to inputs by construction, as the full manuscript equations and any cited prior results on rethermalization timescales are not exhibited in the provided source. The abstract states the thermalization premise and the resulting black-hole mass range as a conclusion without showing a fitted parameter renamed as prediction or an ansatz smuggled via self-citation. This is the expected honest non-finding when no explicit reduction is quotable.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Axion dark matter thermalizes by gravitational self-interactions and forms a Bose-Einstein condensate
- ad hoc to paper Rethermalization during initial collapse transports angular momentum outward sufficiently fast for black-hole formation
Forward citations
Cited by 1 Pith paper
-
Axions explain the formation of supermassive black holes at cosmic dawn
Supermassive black holes form naturally at cosmic dawn when dark matter is axions or axion-like particles with mass above 10^{-16} eV/c².
Reference graph
Works this paper leans on
-
[1]
J. Kormendy and L.C. Ho, Ann. Rev. of Astron. and Astroph. , 51 (2013) 511
work page 2013
-
[2]
A. Kazunori et al. (the EHT Collaboration), Ap. J. Lett. 8 75 (2019) L5, and Ap. J. Lett. 930 (2022) L12
work page 2019
- [3]
-
[4]
G. Agazie et al. (the NANOGrav. Collaboration), Ap. J. Le tt. 951 (2023) L8; D.J. Reardon et al., Ap. J. Lett. 951 (2023) L6; H. Xu et al., Res. Astron. As troph. 23 (2023) 075024; J. Antoniadis et al. (the EPTA Collaboration), arXiv: 2306.16 227
work page 2023
-
[5]
K. Inayoshi, E. Visbal and Z. Haiman, Ann. Rev. of Astron. and Astroph., 58 (2020) 27
work page 2020
-
[6]
S. Balberg and S.L. Shapiro, Phys. Rev. Lett. 88 (2002) 10 1301; J. Pollack, D.N. Spergel and P. Steinhardt, Ap. J. 804 (2015) 2, 131; W.-X. Feng, H.-B. Yu a nd Y.-M. Zhong, Ap. J. Lett. 914 (2021) 2, L26
work page 2002
-
[7]
T. Rindler-Daller, K. Freese, M.H. Montgomery, D. Winge t and B. Paxton, Ap. J. 799 (2015) 210
work page 2015
-
[8]
R. Larson et al., Ap. J. Lett. 953 (2023) L29; A. Bogdan et a l., Nature Atron. 8 (2024) 126; R. Maiolino et al., arXiv:2308.01230; L.J. Furtak et al., ar Xiv: 2308.05735; R. Miaolino et al., Nature 627 (2024) 59
- [9]
- [10]
- [11]
- [12]
-
[13]
J. Preskill, F. Wilczek and M. Wise, Phys. Lett. B120 (19 83) 127; L. Abbott and P. Sikivie, Phys. Lett. B120 (1983) 133; M. Dine and W. Fischler, Phys. Le tt. B120 (1983) 137
work page 1983
- [14]
-
[15]
J.M. Bardeen, J.R. Bond, N. Kaiser and A.S. Szalay, Ap. J . 304 (1986) 15
work page 1986
- [16]
-
[17]
G. Efstatathiou and B.J.T. Jones, MNRAS 186 (1979) 133; J. Barnes and G. Efstathiou, Ap. J. 319 (1987) 575
work page 1979
-
[18]
X. Hernanadez, C. Park, B. Cervantes-Sodi and Y.-Y. Cho i, MNRAS 375 (2007) 163
work page 2007
-
[19]
C.C. Lin, L. Meistel and F.H. Shu, Ap. J. 142 (1965) 1431; Y.B. Zel’dovich, Astron. and Astroph. 5 (1970) 84; J. Binney, Ap. J. 215 (1977) 492
work page 1965
- [20]
-
[21]
F. Ferrarese and D. Merritt, Ap. J. 538 (2000) L9; K. Gebh ardt et al., Ap. J. (2000) L13
work page 2000
-
[22]
R.K. Pathria and P.D. Beale, Statistical Mechanics, 3rd edition, Elsevier 2011, and references therein
work page 2011
- [23]
-
[24]
Weinberg, Gravitation and Cosmology , J
S. Weinberg, Gravitation and Cosmology , J. Wiley and Sons, 1972. 13 x ˙x a) t ≪ tin b) t = tin c) t ≲ tcoll d) t = tcoll FIG. 1: Phase space distribution of cold collisionless part icles during the collpase of a large smooth overdensity near cosmic dawn, at four different times: a) just after the Big Bang, b) when the central part of the overdeisty is at ...
work page 1972
-
[25]
0 0 . 5 1 . 0 1 . 5 2 . 0 2 . 5 3 . 0 r
-
[26]
25 ρ(r, tin) r|M =1 ¯ρ(tin) FIG. 2: Density profile at time tin, when the central part of the overdensity is at turnaround, in units where Mf = 1 and R = 1. In these units the central density ρ(⃗0, t in) = 3 / 4π and the contemporary average cosmological enegy density ¯ρ(tin) = 4 / 3π 3. The average cosmological enegy density is indicated by the horizontal...
-
[27]
0 0 . 2 0 . 4 0 . 6 0 . 8 1 . 0 j 100 102 104 106 108 1010 MBH/M⊙ a) Mf = 3 × 1010 M⊙ b) Mf = 1 × 109 M⊙ c) Mf = 3 × 107 M⊙ FIG. 3: Black hole mass as a function of j ≡ ω intin for three values of Mf . For given Mf there is only a very slight dependence of the black hole mass on tin. The values shown were computed for zcoll = 10 and hence tin = 240 Myr. 16
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.