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arxiv: 2605.30446 · v1 · pith:3WSCYOFQnew · submitted 2026-05-28 · 🌀 gr-qc

Cosmological accretion onto braneworld black holes: a relativistic treatment

Pith reviewed 2026-06-29 05:40 UTC · model grok-4.3

classification 🌀 gr-qc
keywords braneworld black holesprimordial black holesaccretionRandall-Sundrumcosmological evolutionfive-dimensional gravitydark matter
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The pith

Braneworld effects drive far stronger early accretion onto primordial black holes than four-dimensional models allow.

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

The paper re-examines how black holes on a Randall-Sundrum brane pull in cosmological fluid. It combines the Shiromizu-Maeda-Sasaki projection with Michel's relativistic accretion solution to show that five-dimensional corrections extend and intensify the accretion phase at early times. This changes the relation between the mass a black hole starts with and the mass it reaches today, sometimes by several orders of magnitude. A reader would care because the result revises whether light primordial black holes could grow enough to explain dark matter or other observations.

Core claim

Braneworld effects play a significant role in the early Universe, strongly impacting the evolution of light primordial black holes. The mapping between initial conditions and present-day PBH populations is substantially modified by an extended phase of early-time accretion that is significantly more efficient than previously found. For certain regions of parameter space, PBHs that could contribute to the present-day dark matter abundance may have formed with masses below the effective four-dimensional Planck scale. The discrepancy between our black hole masses and the most optimistic previous estimates grows as t^{0.34}, reaching up to ∼10^5 for the smallest M_5 permitted by observations.

What carries the argument

Michel's 1972 relativistic spherical accretion solution projected onto the brane via the Shiromizu-Maeda-Sasaki formalism and Gauss-Codazzi equations, which alters the effective density and velocity of the accreting fluid.

If this is right

  • Light primordial black holes can reach masses large enough to contribute to dark matter even when they form below the four-dimensional Planck scale.
  • The present-day abundance of black holes that formed early is substantially higher than four-dimensional estimates imply.
  • The strongest enhancement occurs for the smallest allowed values of the five-dimensional Planck scale M_5.
  • Accretion remains efficient over a longer interval than in standard cosmology, altering the time at which black holes transition from accretion-dominated to other evolutionary regimes.

Where Pith is reading between the lines

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

  • If the result holds, constraints on primordial black holes as dark matter derived from four-dimensional accretion models would need to be recomputed from scratch.
  • The same formalism could be applied to other early-universe objects whose growth is sensitive to the effective gravitational strength on the brane.
  • Future gravitational-wave or microlensing surveys targeting sub-solar-mass black holes would provide a direct test of the modified growth law.

Load-bearing premise

Michel's 1972 accretion solution together with the braneworld projection equations fully describes the fluid-black hole interaction without further five-dimensional corrections or back-reaction on the brane geometry.

What would settle it

A direct measurement or simulation of primordial black hole masses at the end of the radiation era that fails to show the predicted t^{0.34} growth factor relative to four-dimensional accretion would falsify the central claim.

read the original abstract

Higher-dimensional black holes have been extensively studied over the years, primarily from heuristic and fundamental perspectives or within the context of holographic applications. However, their interaction with ordinary matter confined to the brane is also of particular interest in cosmology. In this work, we revisit accretion within the Randall-Sundrum type II framework, employing the covariant Shiromizu-Maeda-Sasaki formalism together with the Gauss-Codazzi and energy conservation equations. We analyse information propagation in the cosmological fluid and implement a fully relativistic treatment of accretion following Michel's prescription. We find that braneworld effects play a significant role in the early Universe, strongly impacting the evolution of light primordial black holes (PBHs). In particular, the mapping between initial conditions and present-day PBH populations is substantially modified by an extended phase of early-time accretion that is significantly more efficient than previously found. For certain regions of parameter space, PBHs that could contribute to the present-day dark matter abundance may have formed with masses below the effective four-dimensional Planck scale. The discrepancy between our black hole masses and the most optimistic previous estimates grows as $t^{0.34}$-a significant difference that reaches up to several orders of magnitude by the end of the strong-accretion epoch, particularly for black holes that form early and for small values of the fundamental Planck scale $M_5$, reaching up to $\sim 10^5$ for the smallest $M_5$ permitted by observations.

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 / 0 minor

Summary. The paper claims that within the Randall-Sundrum II braneworld, the Shiromizu-Maeda-Sasaki (SMS) formalism combined with Gauss-Codazzi equations and Michel's 1972 relativistic steady-state accretion solution yields substantially more efficient early-universe accretion onto primordial black holes than prior estimates. This produces a mass discrepancy that grows as t^{0.34}, reaching factors up to ~10^5 by the end of the strong-accretion epoch for early-forming PBHs and small M_5, implying that PBHs contributing to present-day dark matter could have formed with initial masses below the effective 4D Planck scale.

Significance. If the central result holds, the work would meaningfully revise the mapping between PBH formation conditions and present-day abundances, expanding the viable parameter space for PBH dark matter and highlighting the importance of braneworld corrections during radiation domination. The explicit use of a covariant 4D effective treatment and relativistic accretion is a methodological strength.

major comments (1)
  1. [Abstract (method paragraph)] Abstract (method paragraph): the central t^{0.34} scaling and the factor-of-10^5 discrepancy are obtained by integrating the Michel accretion rate into the SMS-projected continuity and Einstein equations. The manuscript must explicitly demonstrate that bulk Weyl-tensor contributions beyond the standard dark-radiation term, as well as any back-reaction of the radial inflow on the brane geometry, remain negligible throughout the radiation era when the horizon size approaches the AdS radius set by M_5; otherwise the effective sound speed and capture cross-section used in the integration are not justified.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the detailed and constructive report. The single major comment identifies a necessary justification for the validity of the effective 4D treatment in the regime where the horizon size approaches the AdS radius. We address this point directly below and will revise the manuscript to incorporate the requested demonstration.

read point-by-point responses
  1. Referee: [Abstract (method paragraph)] Abstract (method paragraph): the central t^{0.34} scaling and the factor-of-10^5 discrepancy are obtained by integrating the Michel accretion rate into the SMS-projected continuity and Einstein equations. The manuscript must explicitly demonstrate that bulk Weyl-tensor contributions beyond the standard dark-radiation term, as well as any back-reaction of the radial inflow on the brane geometry, remain negligible throughout the radiation era when the horizon size approaches the AdS radius set by M_5; otherwise the effective sound speed and capture cross-section used in the integration are not justified.

    Authors: We agree that an explicit demonstration of the negligibility of higher-order bulk Weyl contributions and back-reaction is required for the regime in which the black-hole horizon becomes comparable to the AdS radius. The SMS projection already encodes the leading dark-radiation term (the projected Weyl tensor component that behaves as radiation), but the manuscript does not currently quantify the size of the remaining bulk terms or the perturbation to the brane geometry induced by the radial inflow. In the revised version we will add a dedicated subsection (and supporting estimates in an appendix) that compares the magnitude of the neglected Weyl components to the dark-radiation term using the Gauss-Codazzi relations and the characteristic scales of the radiation-dominated era. We will also estimate the back-reaction by comparing the accretion-induced stress-energy perturbation to the background brane tension and curvature scale set by M_5. These estimates will be performed for the parameter ranges (early formation times and smallest observationally allowed M_5) that produce the reported t^{0.34} growth and 10^5 mass discrepancy, thereby confirming that the Michel solution and the adopted sound speed remain applicable. revision: yes

Circularity Check

0 steps flagged

No significant circularity; derivation applies external 1972 Michel solution and SMS formalism to obtain t^{0.34} growth

full rationale

The paper computes the reported mass discrepancy (growing as t^{0.34}, up to 10^5) by inserting Michel's 1972 relativistic accretion solution into the Shiromizu-Maeda-Sasaki projected Einstein equations and Gauss-Codazzi relations on the brane, then integrating the resulting continuity equation for the cosmological fluid. No equation or result is defined in terms of itself, no fitted parameter is relabeled as a prediction, and no load-bearing premise rests on a self-citation whose content is unverified. The t^{0.34} scaling is an output of the integration under the stated assumptions rather than an input by construction, and the cited formalisms (Michel 1972, SMS 2000) are independent of the present authors.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

Abstract-only review prevents exhaustive ledger; the central claim rests on the validity of the SMS formalism and Michel accretion solution applied to RSII, plus the assumption that the five-dimensional Planck scale M_5 is an external input.

free parameters (1)
  • M_5
    Fundamental five-dimensional Planck scale treated as a free parameter bounded by observations; the reported discrepancy reaches 10^5 for its smallest allowed value.
axioms (2)
  • domain assumption Shiromizu-Maeda-Sasaki formalism plus Gauss-Codazzi equations correctly describe the effective four-dimensional dynamics of braneworld black holes.
    Invoked in the method paragraph of the abstract as the framework for the entire calculation.
  • domain assumption Michel's 1972 relativistic accretion solution remains valid when transplanted to the braneworld geometry.
    Explicitly stated as the prescription followed for the accretion treatment.

pith-pipeline@v0.9.1-grok · 5799 in / 1553 out tokens · 25523 ms · 2026-06-29T05:40:40.529035+00:00 · methodology

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Reference graph

Works this paper leans on

52 extracted references · 15 canonical work pages · 12 internal anchors

  1. [1]

    Arkani–Hamed, S

    N. Arkani–Hamed, S. Dimopoulos and G. Dvali,The hierarchy problem and new dimensions at a millimeter,Physics Letters B429(1998) 263–272

  2. [2]

    Randall and R

    L. Randall and R. Sundrum,Large mass hierarchy from a small extra dimension,Physical Review Letters83(1999) 3370–3373

  3. [3]

    Randall and R

    L. Randall and R. Sundrum,An alternative to compactification,Physical Review Letters83 (1999) 4690–4693

  4. [4]

    Green and B.J

    A.M. Green and B.J. Kavanagh,Primordial black holes as a dark matter candidate,Journal of Physics G: Nuclear and Particle Physics48(2021) 043001

  5. [5]

    Escrivà, F

    A. Escrivà, F. Kühnel and Y. Tada,Primordial black holes, inBlack Holes in the Era of Gravitational-Wave Astronomy, p. 261–377, Elsevier (2024), DOI

  6. [6]

    Vennin and D

    C. Byrnes, G. Franciolini, T. Harada, P. Pani and M. Sasaki, eds.,Primordial Black Holes, Springer Series in Astrophysics and Cosmology, Springer (2025), 10.1007/978-981-97-8887-3

  7. [7]

    Hawking,Gravitationally collapsed objects of very low mass,Monthly Notices of the Royal Astronomical Society152(1971) 75

    S. Hawking,Gravitationally collapsed objects of very low mass,Monthly Notices of the Royal Astronomical Society152(1971) 75

  8. [8]

    Aldecoa-Tamayo, C.T

    I. Aldecoa-Tamayo, C.T. Byrnes and D. Seery,Primordial black holes in randall-sundrum: cosmological signatures,Journal of Cosmology and Astroparticle Physics2026(2026) 002

  9. [9]

    Guedens, D

    R. Guedens, D. Clancy and A.R. Liddle,Primordial black holes in braneworld cosmologies: Accretion after formation,Physical Review D66(2002)

  10. [10]

    Primordial black holes in braneworld cosmologies: astrophysical constraints

    D. Clancy, R. Guedens and A.R. Liddle,Primordial black holes in brane world cosmologies: Astrophysical constraints,Phys. Rev. D68(2003) 023507 [astro-ph/0301568]

  11. [11]

    Majumdar,Domination of black hole accretion in brane cosmology,Physical Review Letters90(2003)

    A.S. Majumdar,Domination of black hole accretion in brane cosmology,Physical Review Letters90(2003) . – 25 –

  12. [12]

    Interacting black holes on the brane: the seeding of binaries

    A.S. Majumdar, A. Mehta and J.M. Luck,Interacting black holes on the brane: The Seeding of binaries,Phys. Lett. B607(2005) 219 [astro-ph/0311148]

  13. [13]

    Gravitational lensing in the weak field limit by a braneworld black hole

    A.S. Majumdar and N. Mukherjee,Gravitational lensing in the weak field limit by a braneworld black hole,Mod. Phys. Lett. A20(2005) 2487 [astro-ph/0403405]

  14. [14]

    Braneworld black holes in cosmology and astrophysics

    A.S. Majumdar and N. Mukherjee,Braneworld black holes in cosmology and astrophysics,Int. J. Mod. Phys. D14(2005) 1095 [astro-ph/0503473]

  15. [15]

    Gravitational Waves from Sub-lunar Mass Primordial Black Hole Binaries - A New Probe of Extradimensions

    K.T. Inoue and T. Tanaka,Gravitational waves from sublunar mass primordial black hole binaries: A New probe of extradimensions,Phys. Rev. Lett.91(2003) 021101 [gr-qc/0303058]

  16. [16]

    Constraints on the mass spectrum of primordial black holes and braneworld parameters from the high-energy diffuse photon background

    Y. Sendouda, S. Nagataki and K. Sato,Constraints on the mass spectrum of primordial black holes and braneworld parameters from the high-energy diffuse photon background,Phys. Rev. D 68(2003) 103510 [astro-ph/0309170]

  17. [17]

    Sub-GeV galactic cosmic-ray antiprotons from primordial black holes in the Randall-Sundrum braneworld

    Y. Sendouda, K. Kohri, S. Nagataki and K. Sato,Sub-GeV galactic cosmic-ray antiprotons from PBHs in the Randall-Sundrum braneworld,Phys. Rev. D71(2005) 063512 [astro-ph/0408369]

  18. [18]

    How particle collisions increase the rate of accretion from the cosmological background onto primordial black holes in braneworld cosmology

    V.V. Tikhomirov and Y.A. Tsalkou,How particle collisions increase the rate of accretion from cosmological background onto primordial black holes in braneworld cosmology,Phys. Rev. D72 (2005) 121301 [astro-ph/0510212]

  19. [19]

    Braneworld black holes as gravitational lenses

    E.F. Eiroa,Braneworld black holes as gravitational lenses,Braz. J. Phys.35(2005) 1113 [gr-qc/0511004]

  20. [20]

    Formalism for testing theories of gravity using lensing by compact objects. III: Braneworld gravity

    C.R. Keeton and A.O. Petters,Formalism for testing theories of gravity using lensing by compact objects. III. Braneworld gravity,Phys. Rev. D73(2006) 104032 [gr-qc/0603061]

  21. [21]

    Mass spectrum of primordial black holes from inflationary perturbation in the Randall-Sundrum braneworld: a limit on blue spectra

    Y. Sendouda, S. Nagataki and K. Sato,Mass spectrum of primordial black holes from inflationary perturbation in the randall-sundrum braneworld: a limit on blue spectra,JCAP06 (2006) 003 [astro-ph/0603509]

  22. [22]

    Sendouda,Cosmic rays from primordial black holes in the Randall-Sundrum braneworld, AIP Conf

    Y. Sendouda,Cosmic rays from primordial black holes in the Randall-Sundrum braneworld, AIP Conf. Proc.861(2006) 1023

  23. [23]

    Friedlander, K.J

    A. Friedlander, K.J. Mack, S. Schon, N. Song and A.C. Vincent,Primordial black hole dark matter in the context of extra dimensions,Phys. Rev. D105(2022) 103508 [2201.11761]

  24. [24]

    Friedlander, N

    A. Friedlander, N. Song and A.C. Vincent,Dark matter from higher-dimensional primordial black holes,Phys. Rev. D108(2023) 043523 [2306.01520]

  25. [25]

    Ghoshal, E

    A. Ghoshal, E. Megias, G. Nardini and M. Quiros,Complementary probes of warped extra dimension: Colliders, gravitational waves and primordial black holes from phase transitions, 2025

  26. [26]

    Vitale, G

    G.F. Vitale, G. Lambiase, T.K. Poddar and L. Visinelli,Microscopic primordial black holes as macroscopic dark matter from large extra dimensions, 2026

  27. [27]

    John, S.G

    A.J. John, S.G. Ghosh and S.D. Maharaj,Accretion onto a higher dimensional black hole, Physical Review D88(2013)

  28. [28]

    Bondi,On spherically symmetric accretion,Monthly Notices of the Royal Astronomical Society112(1952) 195

    H. Bondi,On spherically symmetric accretion,Monthly Notices of the Royal Astronomical Society112(1952) 195

  29. [29]

    Harko,Matter accretion by brane-world black holes,Journal of the Korean Physical Society 54(2009) 2583–2594

    T. Harko,Matter accretion by brane-world black holes,Journal of the Korean Physical Society 54(2009) 2583–2594

  30. [30]

    Michel,Accretion of matter by condensed objects,Astrophysics and Space Science15 (1972) 153

    F.C. Michel,Accretion of matter by condensed objects,Astrophysics and Space Science15 (1972) 153

  31. [31]

    Ricotti,Bondi accretion in the early universe,The Astrophysical Journal662(2007) 53–61

    M. Ricotti,Bondi accretion in the early universe,The Astrophysical Journal662(2007) 53–61. – 26 –

  32. [32]

    Shiromizu, K.-i

    T. Shiromizu, K.-i. Maeda and M. Sasaki,The einstein equations on the 3-brane world, Physical Review D62(2000)

  33. [33]

    Maartens,Brane-world gravity,Living Reviews in Relativity7(2004)

    R. Maartens,Brane-world gravity,Living Reviews in Relativity7(2004)

  34. [34]

    Sasankan, M.R

    N. Sasankan, M.R. Gangopadhyay, G.J. Mathews and M. Kusakabe,New observational limits on dark radiation in braneworld cosmology,Physical Review D95(2017)

  35. [35]

    Sasankan, M.R

    N. Sasankan, M.R. Gangopadhyay, G.J. Mathews and M. Kusakabe,Limits on brane-world and particle dark radiation from big bang nucleosynthesis and the cmb,International Journal of Modern Physics E26(2017) 1741007

  36. [36]

    Binétruy, C

    P. Binétruy, C. Deffayet, U. Ellwanger and D. Langlois,Brane cosmological evolution in a bulk with cosmological constant,Physics Letters B477(2000) 285–291

  37. [37]

    Tangherlini,Schwarzschild field in n dimensions and the dimensionality of space problem, Nuovo Cim.27(1963) 636

    F.R. Tangherlini,Schwarzschild field in n dimensions and the dimensionality of space problem, Nuovo Cim.27(1963) 636

  38. [38]

    Gregory, R

    R. Gregory, R. Whisker, K. Beckwith and C. Done,Observing braneworld black holes,Journal of Cosmology and Astroparticle Physics2004(2004) 013–013

  39. [39]

    Brillouin,Wave Propagation and Group Velocity, vol

    L. Brillouin,Wave Propagation and Group Velocity, vol. 8 ofPure and Applied Physics, Academic Press, New York (1960)

  40. [40]

    Maartens and K

    R. Maartens and K. Koyama,Brane-world gravity,Living Reviews in Relativity13(2010)

  41. [41]

    Langlois, R

    D. Langlois, R. Maartens, M. Sasaki and D. Wands,Large-scale cosmological perturbations on the brane,Physical Review D63(2001)

  42. [42]

    Cardoso, T

    A. Cardoso, T. Hiramatsu, K. Koyama and S.S. Seahra,Scalar perturbations in braneworld cosmology,Journal of Cosmology and Astroparticle Physics2007(2007) 008–008

  43. [43]

    Mukohyama,Gauge-invariant gravitational perturbations of maximally symmetric spacetimes,Physical Review D62(2000)

    S. Mukohyama,Gauge-invariant gravitational perturbations of maximally symmetric spacetimes,Physical Review D62(2000)

  44. [44]

    Kodama, A

    H. Kodama, A. Ishibashi and O. Seto,Brane world cosmology: Gauge-invariant formalism for perturbation,Physical Review D62(2000)

  45. [45]

    Shapiro and S.A

    S.L. Shapiro and S.A. Teukolsky,Appendix g: Spherical accretion onto a black hole: The relativistic equations, inBlack Holes, White Dwarfs, and Neutron Stars, pp. 568–575, John Wiley & Sons, Ltd (1983), DOI

  46. [46]

    Tests of the Gravitational Inverse-Square Law below the Dark-Energy Length Scale

    D.J. Kapner, T.S. Cook, E.G. Adelberger, J.H. Gundlach, B.R. Heckel, C.D. Hoyle et al.,Tests of the gravitational inverse-square law below the dark-energy length scale,Phys. Rev. Lett.98 (2007) 021101 [hep-ph/0611184]

  47. [47]

    anti-evaporate

    R. Casadio and C. Germani,Gravitational collapse and black hole evolution: – do holographic black holes eventually “anti-evaporate”? –,Progress of Theoretical Physics114(2005) 23–56

  48. [48]

    Langlois, R

    D. Langlois, R. Maartens and D. Wands,Gravitational waves from inflation on the brane, Physics Letters B489(2000) 259–267

  49. [49]

    Seery and A

    D. Seery and A. Taylor,Consistency relation in general braneworld inflation,Physical Review D71(2005)

  50. [50]

    Gorbunov, V.A

    D.S. Gorbunov, V.A. Rubakov and S.M. Sibiryakov,Gravity waves from inflating brane or mirrors moving in ads5,Journal of High Energy Physics2001(2001) 015–015

  51. [51]

    Tristram, A

    M. Tristram, A. Banday, K. Górski, R. Keskitalo, C. Lawrence, K. Andersen et al.,Improved limits on the tensor-to-scalar ratio using bicep and planck,Physical Review D105(2022)

  52. [52]

    Aghanim, Y

    N. Aghanim, Y. Akrami, M. Ashdown, J. Aumont, C. Baccigalupi, M. Ballardini et al.,Planck 2018 results: Vi. cosmological parameters,Astronomy & Astrophysics641(2020) A6. – 27 –