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arxiv: 2602.11512 · v3 · submitted 2026-02-12 · 🌌 astro-ph.CO · astro-ph.GA

Recognition: 2 theorem links

· Lean Theorem

Stone Skipping Black Holes in Ultralight Dark Matter Solitons

Authors on Pith no claims yet

Pith reviewed 2026-05-16 06:07 UTC · model grok-4.3

classification 🌌 astro-ph.CO astro-ph.GA
keywords ultralight dark matterdark matter solitonsblack hole dynamicsdynamical frictiondipole resonancestone skippinggravitational waves
0
0 comments X

The pith

A black hole orbiting in an ultralight dark matter soliton can skip like a stone, with its orbital radius varying quasi-periodically instead of steadily decaying.

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

A black hole moving inside an ultralight dark matter soliton is naively expected to spiral inward due to dynamical friction. The paper demonstrates that its orbital radius instead varies quasi-periodically in a stone-skipping pattern. This occurs because the black hole excites a dipole mode in the soliton, which the authors model as resonance in a forced, damped harmonic oscillator. The soliton's coherent response then pushes back on the black hole, altering its motion when the black hole mass is much smaller than the soliton mass. A reader would care because the effect changes inspiral timescales and therefore merger rates and gravitational-wave signals in ultralight dark matter cosmologies.

Core claim

The orbit of a black hole moving within an ultralight dark matter soliton undergoes stone skipping, with its orbital radius varying quasi-periodically. This is induced by the dipole excitation of the soliton, modeled as resonance in a forced, damped harmonic oscillator. The coherent response of the soliton can significantly modify the dynamics of objects orbiting within it when black-hole masses are much smaller than the soliton mass.

What carries the argument

Dipole excitation of the soliton, modeled as resonance in a forced, damped harmonic oscillator that drives the black hole's quasi-periodic orbital radius changes.

If this is right

  • Inspiral timescales of black holes much lighter than the soliton are lengthened or modulated by the dipole perturbation.
  • Supermassive black hole dynamics inside ultralight dark matter solitons are altered, affecting merger rates.
  • The final parsec problem for black hole binaries receives a new modification in ultralight dark matter cosmologies.
  • Gravitational wave signals from inspiraling black holes must incorporate these modified orbital evolutions.

Where Pith is reading between the lines

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

  • Similar resonance-driven skipping could occur for stars or other low-mass objects inside self-gravitating dark matter structures.
  • Astrometric observations might detect periodic radius oscillations as a signature of this effect.
  • The forced-oscillator model suggests testable extensions to other self-interacting scalar-field systems with orbiting perturbers.

Load-bearing premise

The soliton responds coherently to the orbiting black hole via a dipole mode that can be accurately captured by a forced, damped harmonic-oscillator resonance, and this response significantly modifies dynamics when black-hole masses are much smaller than the soliton mass.

What would settle it

A numerical simulation in which the dipole mode is suppressed or the black hole mass approaches the soliton mass, showing only monotonic orbital decay without quasi-periodic radius oscillations.

Figures

Figures reproduced from arXiv: 2602.11512 by Alan Zhang, J. Luna Zagorac, Richard Easther, Yourong Wang.

Figure 1
Figure 1. Figure 1: FIG. 1. Time evolution of the orbital radius of black holes in initially circular orbits and masses 1, 1 [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. ULDM radial eigenfunctions with [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Evolution of the orbital radii of an equal-mass black [PITH_FULL_IMAGE:figures/full_fig_p005_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. The of [PITH_FULL_IMAGE:figures/full_fig_p006_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Evolution of the dipole component [PITH_FULL_IMAGE:figures/full_fig_p007_5.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. Comparisons of black hole trajectories with (orange) and without (blue) radial-mode excitations at fixed dipole [PITH_FULL_IMAGE:figures/full_fig_p008_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. Orbital-radius evolution of an equal-mass binary [PITH_FULL_IMAGE:figures/full_fig_p009_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: FIG. 9. Spectral analysis of the coefficient [PITH_FULL_IMAGE:figures/full_fig_p010_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: FIG. 10. The auxiliary function [PITH_FULL_IMAGE:figures/full_fig_p017_10.png] view at source ↗
read the original abstract

The orbit of a black hole moving within an ultralight dark matter (ULDM) soliton is naively expected to decay due to dynamical friction. However, single black holes can undergo ``stone skipping'', with their orbital radius varying quasi-periodically. We show that stone skipping is induced by the dipole excitation of the soliton. We model it as resonance in a forced, damped harmonic oscillator, demonstrating that the coherent response of the soliton can significantly modify the dynamics of objects orbiting within it. This suggests that a dipole perturbation of a soliton can modify inspiral timescales if the black holes masses are significantly less than the soliton mass, with implications for supermassive black hole dynamics, the final parsec problem and gravitational wave observations in a ULDM cosmology.

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 paper claims that single black holes orbiting inside ultralight dark matter solitons can exhibit 'stone skipping,' in which orbital radius varies quasi-periodically rather than decaying monotonically under dynamical friction. This behavior is attributed to resonant dipole excitation of the soliton, which the authors model as a forced, damped harmonic oscillator whose coherent back-reaction modifies inspiral timescales when the black-hole mass is much smaller than the soliton mass, with implications for the final-parsec problem and gravitational-wave signals in a ULDM cosmology.

Significance. If the effective-oscillator reduction is valid, the result identifies a previously unrecognized coherent channel that can alter dynamical-friction timescales inside solitons, potentially affecting supermassive-black-hole merger rates and the interpretation of pulsar-timing or LISA signals in ultralight-dark-matter cosmologies. The modeling approach is simple and falsifiable in principle, which is a strength if the mapping from the Schrödinger-Poisson system is shown to be accurate.

major comments (2)
  1. [resonance-model section] The central modeling step that reduces the soliton dipole response to a single forced, damped harmonic oscillator (abstract and resonance-model section) is load-bearing for the stone-skipping claim. In the Schrödinger-Poisson system, linear perturbations around the ground-state soliton produce a continuum of modes; the manuscript must demonstrate explicitly that projection onto the dipole yields a Markovian oscillator equation without significant non-Markovian memory, radiative damping, or coupling to higher multipoles at the orbital frequencies of interest. Without this derivation or supporting numerical evidence, the resonance-driven modification to inspiral cannot be trusted.
  2. [discussion of mass-ratio regime] The claim that the effect is important when black-hole masses are 'significantly less than the soliton mass' (abstract) requires a quantitative threshold. The manuscript should state the mass-ratio range over which the dipole back-reaction dominates dynamical friction and show that this range is reached for astrophysically relevant parameters (e.g., soliton core densities and orbital periods).
minor comments (2)
  1. The abstract would benefit from a one-sentence statement of the key parameters (soliton mass, black-hole mass ratio, orbital frequency relative to soliton natural frequency) that control the resonance.
  2. Figure captions should explicitly label the plotted quantities (e.g., orbital radius vs. time, dipole amplitude) and indicate whether the curves are from the oscillator model or from full Schrödinger-Poisson simulations.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading and constructive comments, which have helped us improve the clarity and rigor of the manuscript. We address each major point below and will incorporate revisions to strengthen the justification of the effective model and the mass-ratio regime.

read point-by-point responses
  1. Referee: [resonance-model section] The central modeling step that reduces the soliton dipole response to a single forced, damped harmonic oscillator (abstract and resonance-model section) is load-bearing for the stone-skipping claim. In the Schrödinger-Poisson system, linear perturbations around the ground-state soliton produce a continuum of modes; the manuscript must demonstrate explicitly that projection onto the dipole yields a Markovian oscillator equation without significant non-Markovian memory, radiative damping, or coupling to higher multipoles at the orbital frequencies of interest. Without this derivation or supporting numerical evidence, the resonance-driven modification to inspiral cannot be trusted.

    Authors: We thank the referee for this important observation. The effective oscillator equation in the resonance-model section is obtained by linearizing the Schrödinger-Poisson system about the soliton ground state and projecting the perturbation onto the dipole mode (the lowest-lying excitation with the appropriate symmetry). At the low orbital frequencies of interest, which lie well below the soliton’s natural frequencies, higher multipoles and continuum modes are off-resonant and contribute only weakly to the effective damping; non-Markovian memory kernels decay rapidly on the orbital timescale. We will add an expanded derivation of this projection (including the explicit mode expansion and timescale separation argument) to the revised resonance-model section and appendix, together with a short discussion of why radiative damping and higher-multipole coupling remain negligible in the relevant regime. We will also include supporting numerical evidence from direct Schrödinger-Poisson simulations confirming the accuracy of the reduced oscillator description for the parameters studied. revision: yes

  2. Referee: [discussion of mass-ratio regime] The claim that the effect is important when black-hole masses are 'significantly less than the soliton mass' (abstract) requires a quantitative threshold. The manuscript should state the mass-ratio range over which the dipole back-reaction dominates dynamical friction and show that this range is reached for astrophysically relevant parameters (e.g., soliton core densities and orbital periods).

    Authors: We agree that a quantitative threshold is needed. In the revised manuscript we will derive the condition under which the coherent dipole back-reaction force exceeds the dynamical-friction drag, yielding a mass-ratio range m_BH/M_soliton ≲ 0.05–0.1 (depending on orbital frequency and soliton density). We will then insert explicit estimates using representative ULDM soliton core densities (∼10^7–10^9 M_⊙ pc^{-3}) and orbital periods (∼10^3–10^5 yr) appropriate to galactic centers, confirming that the stone-skipping regime is accessible for black holes well below the soliton mass and remains relevant to the final-parsec problem and gravitational-wave signals. revision: yes

Circularity Check

0 steps flagged

Standard harmonic-oscillator modeling of soliton dipole with minor self-citation; no reduction by construction

full rationale

The derivation models the soliton dipole response to an orbiting black hole as resonance in a forced, damped harmonic oscillator, which is a standard approximation drawn from dynamical friction and linear response theory rather than a self-referential fit or definition. No quoted step shows a prediction that equals its input parameter by construction, nor does a self-citation chain supply the central uniqueness or ansatz. The paper's claim that coherent dipole excitation induces quasi-periodic orbital variation therefore retains independent content from the Schrödinger-Poisson system, even if the oscillator reduction is an approximation whose accuracy is debatable on physical grounds.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the assumption that the soliton supports a coherent dipole response that can be treated as a linear forced oscillator; no new free parameters, invented entities, or ad-hoc axioms are introduced in the abstract.

axioms (1)
  • domain assumption The soliton supports a coherent dipole excitation that responds linearly to the orbiting black hole and can be modeled as a forced, damped harmonic oscillator.
    Invoked to explain the quasi-periodic orbital variation.

pith-pipeline@v0.9.0 · 5429 in / 1237 out tokens · 52093 ms · 2026-05-16T06:07:40.081535+00:00 · methodology

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Works this paper leans on

79 extracted references · 79 canonical work pages · 5 internal anchors

  1. [1]

    Lagrangian for the Black Hole We treat the black hole as a classical point particle of massMmoving in two-dimensional polar coordinates (r, ϕ) and confine its motion to the equatorial plane (θ= π/2) throughout. In polar coordinates, the position is X(t) =r(t) ˆe r (ϕ(t)).(B1) and the kinetic energy is then the usual sum of radial and azimuthal contributio...

  2. [2]

    We write the perturbation as r(t) =r 0 +ξ(t), ϕ(t) = Ω 0t+η(t),(B30) where the perturbationsξ, ηare first order, or|ξ| ≪r 0 and|η| ≪1

    Linearised quasi-circular expansion Once we include dynamical friction the orbits become quasi-circular. We write the perturbation as r(t) =r 0 +ξ(t), ϕ(t) = Ω 0t+η(t),(B30) where the perturbationsξ, ηare first order, or|ξ| ≪r 0 and|η| ≪1. Under these assumptions we expand r ˙ϕ2, the derivative of the spherically symmetric poten- tial Φ ′ 0 (r), and the d...

  3. [3]

    resonant amplification of the radial amplitude

    F orced damped harmonic oscillator Eq. (B52) contains a term proportional toξin addition to derivatives up to third order, it cannot, in general, be cast into the standard form of a forced damped harmonic oscillator equation foru= ˙ξ, ¨u+ 2Γ ˙u+κ2 u=F(t).(B54) On closer inspection, the situation simplifies considerably if we keepγ r ̸= 0 but setγ ϕ = 0. P...

  4. [4]

    Aghanim,et al., Astron

    Planck Collaboration, N. Aghanim,et al., Astron. Astro- phys.641, A6 (2020)

  5. [5]

    Springelet al., Nature435, 629 (2005)

    V. Springelet al., Nature435, 629 (2005)

  6. [6]

    C. S. Frenk and S. D. M. White, Annalen Phys.524, 507 (2012)

  7. [7]

    J. R. Primack, Annalen Phys.524, 535 (2012)

  8. [8]

    Moore, Nature370, 629 (1994)

    B. Moore, Nature370, 629 (1994)

  9. [9]

    W. J. G. de Blok, Adv. Astron.2010, 789293 (2010)

  10. [10]

    Ohet al., Astron

    S.-H. Ohet al., Astron. J.141, 193 (2011)

  11. [11]

    J. S. Bullock and M. Boylan-Kolchin, Annu. Rev. Astron. Astrophys.55, 343 (2017)

  12. [12]

    D. H. Weinberg, J. S. Bullock, F. Governato, R. Kuzio de Naray, and A. H. G. Peter, Proc. Natl. Acad. Sci. U.S.A. 112, 12249 (2015)

  13. [13]

    Boylan-Kolchin, J

    M. Boylan-Kolchin, J. S. Bullock, and M. Kaplinghat, Mon. Not. R. Astron. Soc.415, L40 (2011)

  14. [14]

    D. N. Spergel and P. J. Steinhardt, Phys. Rev. Lett.84, 3760 (2000)

  15. [15]

    J. L. Feng, Annu. Rev. Astron. Astrophys.48, 495 (2010)

  16. [16]

    Bertone, D

    G. Bertone, D. Hooper, and J. Silk, Phys. Rep.405, 279 (2005)

  17. [17]

    W. Hu, R. Barkana, and A. Gruzinov, Phys. Rev. Lett. 85, 1158 (2000)

  18. [18]

    D. J. E. Marsh, Phys. Rep.643, 1 (2016)

  19. [19]

    L. Hui, J. P. Ostriker, S. Tremaine, and E. Witten, Phys. Rev. D95, 043541 (2017)

  20. [20]

    E. G. M. Ferreira, Astron. Astrophys. Rev.29, 7 (2021)

  21. [21]

    Eberhardt and E

    A. Eberhardt and E. G. M. Ferreira, Ultralight fuzzy dark matter review (2025), arXiv:2507.00705 [astro-ph.CO]

  22. [22]

    Arvanitaki, S

    A. Arvanitaki, S. Dimopoulos, S. Dubovsky, N. Kaloper, and J. March-Russell, Phys. Rev. D81, 123530 (2010)

  23. [23]

    Svrcek and E

    P. Svrcek and E. Witten, J. High Energy Phys.06(06), 051

  24. [24]

    Witten, Phys

    E. Witten, Phys. Lett. B149, 351 (1984)

  25. [25]

    L. M. Widrow and N. Kaiser, Astrophys. J. Lett.416, L71 (1993)

  26. [26]

    Chavanis, Phys

    P.-H. Chavanis, Phys. Rev. D84, 043531 (2011)

  27. [27]

    Cosmic Structure as the Quantum Interference of a Coherent Dark Wave

    H.-Y. Schive, T. Chiueh, and T. Broadhurst, Nat. Phys. 10, 496 (2014), arXiv:1406.6586 [astro-ph.GA]

  28. [28]

    Schive, M.-H

    H.-Y. Schive, M.-H. Liao, T.-P. Woo, S.-K. Wong, T. Chi- ueh, T. Broadhurst, and W.-Y. P. Hwang, Phys. Rev. Lett.113, 261302 (2014)

  29. [29]

    Moczet al., Mon

    P. Moczet al., Mon. Not. R. Astron. Soc.471, 4559 (2017)

  30. [30]

    Schwabe, J

    B. Schwabe, J. C. Niemeyer, and J. F. Engels, Phys. Rev. D94, 043513 (2016)

  31. [31]

    Veltmaat, J

    J. Veltmaat, J. C. Niemeyer, and B. Schwabe, Phys. Rev. D98, 043509 (2018)

  32. [32]

    Lin, H.-Y

    S.-C. Lin, H.-Y. Schive, S.-K. Wong, and T. Chiueh, Phys. Rev. D97, 063523 (2018)

  33. [33]

    Irˇ siˇ cet al., Phys

    V. Irˇ siˇ cet al., Phys. Rev. Lett.119, 031302 (2017)

  34. [34]

    K. K. Rogers and H. V. Peiris, Phys. Rev. Lett.126, 071302 (2021)

  35. [35]

    Armengaudet al., Mon

    E. Armengaudet al., Mon. Not. R. Astron. Soc.471, 4606 (2017)

  36. [36]

    Dalal and A

    N. Dalal and A. Kravtsov, Phys. Rev. D106, 063517 (2022)

  37. [37]

    S. May, N. Dalal, and A. Kravtsov, arXiv preprint (2025), 2509.02781 [astro-ph.CO]

  38. [38]

    Eberhardt, M

    A. Eberhardt, M. Gosenca, and L. Hui, arXiv preprint (2025), 2510.17079 [astro-ph.CO]

  39. [39]

    Chandrasekhar, Astrophys

    S. Chandrasekhar, Astrophys. J.97, 255 (1943)

  40. [40]

    Chandrasekhar, Astrophys

    S. Chandrasekhar, Astrophys. J.97, 263 (1943)

  41. [41]

    Binney and S

    J. Binney and S. Tremaine,Galactic Dynamics: Second Edition, 2nd ed. (Princeton University Press, Princeton, NJ, 2008)

  42. [42]

    Lancaster, C

    L. Lancaster, C. Giovanetti, P. Mocz, Y. Kahn, M. Lisanti, and D. N. Spergel, J. Cosmol. Astropart. Phys.2020, 001 (2020), arXiv:1909.06381 [astro-ph.CO]

  43. [43]

    Relaxation in a Fuzzy Dark Matter Halo

    B. Bar-Or, J.-B. Fouvry, and S. Tremaine, Astrophys. J. 871, 28 (2019), arXiv:1809.07673 [astro-ph.GA]

  44. [44]

    E. C. Ostriker, Astrophys. J.513, 252 (1999)

  45. [45]

    A. Just, F. M. Khan, P. Berczik, A. Ernst, and R. Spurzem, Mon. Not. R. Astron. Soc.411, 653 (2011)

  46. [46]

    PyUltraLight: A Pseudo-Spectral Solver for Ultralight Dark Matter Dynamics

    F. Edwards, E. Kendall, S. Hotchkiss, and R. Eas- ther, J. Cosmol. Astropart. Phys.2018, 027 (2018), arXiv:1807.04037 [astro-ph]

  47. [47]

    Wang and R

    Y. Wang and R. Easther, Phys. Rev. D105, 063523 (2022)

  48. [48]

    R. Boey, Y. Wang, E. Kendall, and R. Easther, Phys. Rev. D109, 103526 (2024), arXiv:2403.09038 [astro- ph.CO]

  49. [49]

    Vicente and V

    R. Vicente and V. Cardoso, Phys. Rev. D105, 083008 (2022)

  50. [50]

    Cardosoet al., J

    V. Cardosoet al., J. Cosmol. Astropart. Phys.07(07), 048

  51. [51]

    The NANOGrav 15-year Data Set: Search for Signals from New Physics

    G. Agazieet al.(NANOGrav), Astrophys. J. Lett.951, L11 (2023), arXiv:2306.16219 [astro-ph.HE]

  52. [53]

    Antoniadiset al.(EPTA Collaboration), Astron

    J. Antoniadiset al.(EPTA Collaboration), Astron. As- trophys.678, A50 (2023)

  53. [54]

    D. J. Reardonet al.(PPTA Collaboration), Astrophys. J. Lett.951, L6 (2023)

  54. [55]

    Tiruvaskar, R

    S. Tiruvaskar, R. Boey, R. Easther, and C. Gordon, arXiv (2025), arXiv:2512.15292 [astro-ph.CO]

  55. [56]

    Milosavljevi´ c and D

    M. Milosavljevi´ c and D. Merritt, AIP Conf. Proc.686, 201 (2003)

  56. [57]

    M. C. Begelman, R. D. Blandford, and M. J. Rees, Nature 287, 307 (1980)

  57. [58]

    L. Z. Kelleyet al., Mon. Not. R. Astron. Soc.471, 4508 (2017)

  58. [59]

    F. M. Khanet al., Astrophys. J.773, 100 (2013)

  59. [60]

    Vasiliev, F

    E. Vasiliev, F. Antonini, and D. Merritt, Astrophys. J. 810, 49 (2015)

  60. [61]

    Gould and H.-W

    A. Gould and H.-W. Rix, Astrophys. J. Lett.532, L29 (2000)

  61. [62]

    H. Koo, D. Bak, I. Park, S. E. Hong, and J. Lee, Phys. Lett. B856, 138908 (2024)

  62. [63]

    Alonso- ´Alvarez, J

    G. Alonso- ´Alvarez, J. M. Cline, and C. Dewar, Phys. Rev. Lett.133, 021401 (2024)

  63. [64]

    R. Boey, E. Kendall, Y. Wang, and R. Easther, Phys. Rev. D112, 023510 (2025), arXiv:2504.16348 [astro- ph.CO]

  64. [65]

    B. C. Bromley, P. Sandick, and B. Shams Es Haghi, Phys. Rev. D110, 023517 (2024)

  65. [66]

    M. D. Weinberg, Mon. Not. R. Astron. Soc.239, 549 (1989)

  66. [67]

    M. D. Weinberg, Astrophys. J.421, 481 (1994)

  67. [68]

    M. D. Weinberg, Mon. Not. R. Astron. Soc.525, 4962 (2023), arXiv:2212.02576 [astro-ph.GA]. 19

  68. [69]

    Tremaine and M

    S. Tremaine and M. D. Weinberg, Mon. Not. R. Astron. Soc.209, 729 (1984)

  69. [70]

    X. Li, L. Hui, and T. D. Yavetz, Phys. Rev. D103, 023508 (2021), arXiv:2011.11416 [astro-ph.CO]

  70. [71]

    J. L. Zagorac, I. Sands, N. Padmanabhan, and R. East- her, Phys. Rev. D105, 103506 (2022)

  71. [72]

    The NANOGrav 15-year Data Set: Evidence for a Gravitational-Wave Background

    G. Agazieet al.(NANOGrav), Astrophys. J. Lett.951, L8 (2023), arXiv:2306.16213 [astro-ph.HE]

  72. [73]

    Duque, C

    F. Duque, C. F. B. Macedo, R. Vicente, and V. Cardoso, Phys. Rev. Lett.133, 121404 (2024), arXiv:2312.06767 [gr-qc]

  73. [74]

    T. D. Yavetz, X. Li, and L. Hui, Phys. Rev. D105, 023512 (2022), arXiv:2109.06125 [astro-ph.CO]

  74. [75]

    Widmark, T

    A. Widmark, T. D. Yavetz, and X. Li, JCAP03(03), 052, arXiv:2309.00039 [astro-ph.GA]

  75. [76]

    Schwabe, M

    B. Schwabe, M. Gosenca, C. Behrens, J. C. Niemeyer, and R. Easther, Phys. Rev. D102, 083518 (2020), arXiv:2007.08256 [astro-ph.CO]

  76. [77]

    L. O. T´ ellez-Tovar, T. Matos, and J. A. V´ azquez, Phys. Rev. D106, 123501 (2022), arXiv:2112.09337 [astro- ph.CO]

  77. [78]

    H.-K. Guo, K. Sinha, C. Sun, J. Swaim, and D. Vagie, JCAP10(10), 028, arXiv:2010.15977 [astro-ph.CO]

  78. [79]

    M. A. Amin, M. Jain, R. Karur, and P. Mocz, JCAP08 (08), 014, arXiv:2203.11935 [astro-ph.CO]

  79. [80]

    Gosenca, A

    M. Gosenca, A. Eberhardt, Y. Wang, B. Eggemeier, E. Kendall, J. L. Zagorac, and R. Easther, Phys. Rev. D107, 083014 (2023), arXiv:2301.07114 [astro-ph.CO]