pith. machine review for the scientific record. sign in

arxiv: 2512.01694 · v2 · submitted 2025-12-01 · 🌀 gr-qc

Recognition: 2 theorem links

· Lean Theorem

Quasinormal modes of Reissner-Nordstr\"om-AdS black holes under physical field-vanishing boundary conditions

Authors on Pith no claims yet

Pith reviewed 2026-05-17 03:09 UTC · model grok-4.3

classification 🌀 gr-qc
keywords quasinormal modesReissner-Nordstrom-AdSboundary conditionsblack hole perturbationsAdS spacetimeparity modeselectromagnetic perturbations
0
0 comments X

The pith

A physical field-vanishing boundary condition for RN-AdS black holes requires both metric and electromagnetic perturbations to vanish at the AdS boundary.

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

The paper introduces the physical field-vanishing boundary condition motivated by keeping the boundary metric undeformed and eliminating electromagnetic energy flux at the AdS boundary. This condition is applied to the coupled metric-electromagnetic perturbations of Reissner-Nordström-AdS black holes. Using perturbation reconstruction formulas, the authors convert the condition into Dirichlet-type requirements on the master functions for odd-parity modes and Robin-type requirements for even-parity modes. They then compute the quasinormal frequencies and report new features in the resulting spectrum. Readers would care because boundary conditions control how black holes respond to perturbations in AdS space, directly shaping stability analyses and dynamical properties.

Core claim

The central claim is that the physical field-vanishing boundary condition, which demands that both the metric and electromagnetic field-strength perturbations vanish at the AdS boundary, translates via perturbation reconstruction formulas into Dirichlet boundary conditions for odd-parity modes and Robin boundary conditions for even-parity modes on the master functions, allowing computation of the quasinormal frequencies of RN-AdS black holes and revealing new spectral features.

What carries the argument

The physical field-vanishing (PFV) condition, which enforces vanishing of both metric and electromagnetic field-strength perturbations at the AdS boundary to handle the coupled system consistently.

If this is right

  • Quasinormal frequencies of RN-AdS black holes display new spectral features under the PFV boundary conditions.
  • The PFV prescription extends to other multifield perturbation systems in asymptotically AdS spacetimes.
  • Master functions obey Dirichlet-type conditions for odd-parity modes and Robin-type conditions for even-parity modes.

Where Pith is reading between the lines

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

  • The translation of PFV conditions through perturbation reconstruction formulas offers a systematic route for setting boundary conditions in other charged or multi-field AdS black hole models.
  • If the new spectral features persist across charge values, they may alter expectations for how charge influences ringing behavior compared with neutral AdS cases.

Load-bearing premise

The two guiding principles of non-deformation of the boundary metric and vanishing electromagnetic energy flux together define the physically correct boundary condition for the coupled metric-electromagnetic system.

What would settle it

An explicit calculation demonstrating that the electromagnetic energy flux fails to vanish or that the boundary metric deforms under the proposed conditions would falsify the choice of physical field-vanishing boundary conditions.

Figures

Figures reproduced from arXiv: 2512.01694 by Ding-fang Zeng, Hui-Fa Liu, Qi Su.

Figure 1
Figure 1. Figure 1: FIG. 1. Left, the two lowest purely imaginary-frequency modes of master function [PITH_FULL_IMAGE:figures/full_fig_p007_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Quasinormal frequencies of the master function [PITH_FULL_IMAGE:figures/full_fig_p008_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. The real (left) and imaginary (right) parts of quasinormal frequencies computed from master function [PITH_FULL_IMAGE:figures/full_fig_p008_3.png] view at source ↗
read the original abstract

Boundary conditions play a key role in determining the perturbation behavior of a black hole. Motivated by two guiding principles for single-field perturbations -- the non-deformation of the boundary metric and the vanishing of electromagnetic energy flux at the AdS boundary -- we impose a boundary condition for Reissner-Nordstr\"om-AdS (RN-AdS) black holes requiring both the metric and electromagnetic field-strength perturbations to vanish at the AdS boundary, which we term the physical field-vanishing (PFV) condition. Using the formulas for perturbation reconstruction, we translate the PFV condition into boundary conditions on the master functions: Dirichlet-type for odd-parity modes and Robin-type for even-parity modes. With these boundary conditions, we compute the quasinormal frequencies of RN-AdS black holes and identify new spectral features. The PFV prescription introduced here could be applied to other multifield perturbation systems in asymptotically AdS spacetimes.

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 introduces the physical field-vanishing (PFV) boundary condition for perturbations of Reissner-Nordström-AdS black holes, requiring both metric and electromagnetic field-strength perturbations to vanish at the AdS boundary. This is motivated by the principles of non-deformation of the boundary metric and vanishing electromagnetic energy flux. Using perturbation reconstruction formulas, the PFV condition is mapped to Dirichlet-type boundary conditions for odd-parity modes and Robin-type conditions for even-parity modes on the master functions. The authors then compute the quasinormal frequencies under these conditions and report new spectral features, proposing the prescription for other multifield systems in AdS.

Significance. If the translation to master-function boundary conditions is shown to be consistent and the new spectral features are robust under numerical checks, the work could supply a physically motivated alternative to conventional boundary conditions for coupled gravitational-electromagnetic perturbations in asymptotically AdS spacetimes, with possible relevance to holographic applications and stability studies.

major comments (2)
  1. [Boundary condition translation and Q=0 limit discussion] The manuscript must explicitly verify that the even-parity Robin boundary condition reduces to the standard known boundary condition for Schwarzschild-AdS quasinormal modes in the Q=0 limit, where the electromagnetic sector decouples. Without this check, the reported new spectral features risk being artifacts of an inconsistent coupled-system boundary condition rather than genuine physical effects.
  2. [Numerical computation of quasinormal frequencies] Provide the explicit master equations, the precise form of the Dirichlet and Robin conditions derived from the PFV prescription, and details of the numerical method (including convergence tests and error estimates) used to compute the quasinormal frequencies. These elements are required to substantiate the central claim of new spectral features.
minor comments (2)
  1. Clarify the notation for the master functions and ensure all reconstruction formulas are stated with equation numbers for reproducibility.
  2. Include comparisons of the computed frequencies with existing results for RN-AdS under standard boundary conditions to highlight the differences introduced by PFV.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments. We address each major comment below and have revised the manuscript to incorporate the requested clarifications and details.

read point-by-point responses
  1. Referee: The manuscript must explicitly verify that the even-parity Robin boundary condition reduces to the standard known boundary condition for Schwarzschild-AdS quasinormal modes in the Q=0 limit, where the electromagnetic sector decouples. Without this check, the reported new spectral features risk being artifacts of an inconsistent coupled-system boundary condition rather than genuine physical effects.

    Authors: We agree that an explicit check in the Q=0 limit is necessary to confirm consistency. In the revised manuscript we have added a dedicated subsection demonstrating that the even-parity Robin boundary condition derived from the PFV prescription reduces precisely to the standard boundary condition used for Schwarzschild-AdS perturbations when the charge vanishes and the electromagnetic sector decouples. This verification supports that the new spectral features arise from the coupled system rather than from an inconsistent formulation. revision: yes

  2. Referee: Provide the explicit master equations, the precise form of the Dirichlet and Robin conditions derived from the PFV prescription, and details of the numerical method (including convergence tests and error estimates) used to compute the quasinormal frequencies. These elements are required to substantiate the central claim of new spectral features.

    Authors: We appreciate the request for greater explicitness. The revised manuscript now contains the full set of master equations for both parity sectors, the exact mathematical expressions for the Dirichlet-type conditions (odd parity) and Robin-type conditions (even parity) obtained from the PFV prescription, and an expanded numerical-methods section that describes the pseudospectral implementation together with convergence tests and error estimates for the reported quasinormal frequencies. revision: yes

Circularity Check

0 steps flagged

No circularity: PFV boundary conditions derived from independent physical principles

full rationale

The paper motivates the physical field-vanishing (PFV) boundary condition directly from two stated guiding principles (non-deformation of the boundary metric and vanishing electromagnetic energy flux at the AdS boundary) and then translates it via perturbation reconstruction formulas into Dirichlet/Robin conditions on the master functions. The quasinormal frequencies are subsequently computed from these conditions. No step reduces the reported spectra or new features to a fit, a self-citation chain, or a definition that presupposes the output; the derivation chain remains self-contained against external benchmarks and does not exhibit any of the enumerated circularity patterns.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The claim rests on the Einstein-Maxwell equations in asymptotically AdS spacetime and on the two guiding physical principles used to motivate the PFV condition.

axioms (2)
  • standard math Einstein-Maxwell theory governs the background RN-AdS geometry and its linear perturbations
    Invoked throughout the abstract as the framework for defining quasinormal modes.
  • domain assumption The non-deformation of the boundary metric and the vanishing of electromagnetic energy flux are the appropriate physical requirements at the AdS boundary
    These two principles are stated as the motivation for imposing the PFV condition.

pith-pipeline@v0.9.0 · 5469 in / 1365 out tokens · 42250 ms · 2026-05-17T03:09:36.610461+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.

  • IndisputableMonolith/Foundation/AlexanderDuality.lean alexander_duality_circle_linking unclear
    ?
    unclear

    Relation between the paper passage and the cited Recognition theorem.

    We impose a boundary condition for Reissner-Nordström-AdS (RN-AdS) black holes requiring both the metric and electromagnetic field-strength perturbations to vanish at the AdS boundary, which we term the physical field-vanishing (PFV) condition. Using the formulas for perturbation reconstruction, we translate the PFV condition into boundary conditions on the master functions: Dirichlet-type for odd-parity modes and Robin-type for even-parity modes.

  • IndisputableMonolith/Cost/FunctionalEquation.lean washburn_uniqueness_aczel unclear
    ?
    unclear

    Relation between the paper passage and the cited Recognition theorem.

    The master equations take the Schrödinger-like form [∂²/∂r*² − ∂²/∂t² − V] Ψ = 0 ... with effective potentials V_odd/even_i(r)

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 1 Pith paper

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

  1. Gravitational-Bumblebee perturbations: Exact decoupling and isospectrality

    gr-qc 2026-05 unverdicted novelty 7.0

    Bumblebee gravity perturbations decouple exactly into gravitational and vector sectors, with gravitational modes dynamically immune to Lorentz violation and odd-even parities strictly isospectral.

Reference graph

Works this paper leans on

63 extracted references · 63 canonical work pages · cited by 1 Pith paper · 1 internal anchor

  1. [1]

    Chandrasekhar, The Mathematical Theory of Black Holes (Oxford University Press, New York, 1983)

    S. Chandrasekhar, The Mathematical Theory of Black Holes (Oxford University Press, New York, 1983)

  2. [2]

    H. P. Nollert, TOPICAL REVIEW: Quasinormal modes: The characteristic ‘sound’ of black holes and neutron stars, Classical Quantum Gravity16, R159 (1999)

  3. [3]

    K. D. Kokkotas and B. G. Schmidt, Quasinormal modes of stars and black holes, Living Rev. Relativity2, 2 (1999)

  4. [4]

    Berti, V

    E. Berti, V. Cardoso, and A. O. Starinets, Quasinormal modes of black holes and black branes, Classical Quan- tum Gravity26, 163001 (2009)

  5. [5]

    R. A. Konoplya and A. Zhidenko, Quasinormal modes of black holes: From astrophysics to string theory, Rev. Mod. Phys.83, 793 (2011)

  6. [6]

    S. V. Bolokhov and M. Skvortsova, Review of an- alytic results on quasinormal modes of black holes, arXiv:2504.05014

  7. [7]

    Black hole spectroscopy: from theory to experiment

    E. Bertiet al.Black hole spectroscopy: from theory to experiment, arXiv:2505.23895

  8. [8]

    Bourg, R

    P. Bourg, R. Panosso Macedo, A. Spiers, B. Leather, B. Bonga, and A. Pound, Quadratic quasinormal mode dependence on linear mode parity, Phys. Rev. Lett.134, 061401 (2025)

  9. [9]

    Bourg, R

    P. Bourg, R. Panosso Macedo, A. Spiers, B. Leather, B. Béatrice, and A. Pound, Quadratic quasinormal modes at null infinity on a Schwarzschild spacetime, Phys. Rev. D112, 044049 (2025)

  10. [10]

    G. T. Horowitz and V. E. Hubeny, Quasinormal modes of AdSblackholesandtheapproachtothermalequilibrium, Phys. Rev. D62, 024027 (2000)

  11. [11]

    Cardoso and J

    V. Cardoso and J. P. S. Lemos, Quasinormal modes of Schwarzschildanti-deSitterblackholes: Electromagnetic 10 andgravitationalperturbations, Phys.Rev.D64, 084017 (2001)

  12. [12]

    B. Wang, C. Y. Lin, and E. Abdalla, Quasinormal modes of Reissner-Nordstrom anti-de Sitter black holes, Phys. Lett. B481, 79-88 (2000)

  13. [13]

    Berti and K

    E. Berti and K. D. Kokkotas, Quasinormal modes of Reissner-Nordström-anti-de Sitter black holes: Scalar, electromagnetic and gravitational perturbations, Phys. Rev. D67, 064020 (2003)

  14. [14]

    Cardoso, Ó

    V. Cardoso, Ó. J. C. Dias, G. S. Hartnett, L. Lehner, and J. E. Santos, Holographic thermalization, quasinormal modes and superradiance in Kerr-AdS, JHEP04, 183 (2014)

  15. [15]

    Michalogiorgakis and S

    G. Michalogiorgakis and S. S. Pufu, Low-lying gravita- tional modes in the scalar sector of the global AdS(4) black hole, JHEP02, 023 (2007)

  16. [16]

    Kodama, A

    H. Kodama, A. Ishibashi, and O. Seto, Brane world cosmology: Gauge invariant formalism for perturbation, Phys. Rev. D62, 064022 (2000),

  17. [17]

    Kodama and A

    H. Kodama and A. Ishibashi, A master equation for grav- itational perturbations of maximally symmetric black holes in higher dimensions, Prog. Theor. Phys.110, 701 (2003),

  18. [18]

    Ishibashi and H

    A. Ishibashi and H. Kodama, Stability of higher dimen- sional Schwarzschild black holes, Prog. Theor. Phys.110, 901 (2003),

  19. [19]

    Kodama and A

    H. Kodama and A. Ishibashi, Master equations for per- turbations of generalized static black holes with charge in higher dimensions, Prog. Theor. Phys.111, 29 (2004),

  20. [20]

    Ó. J. C. Dias and J. E. Santos, Boundary conditions for Kerr-AdS perturbations, JHEP10, 156 (2013)

  21. [21]

    M. Wang, C. Herdeiro, and M. O. P. Sampaio, Maxwell perturbations on asymptotically anti–de Sitter space- times: Generic boundary conditions and a new branch of quasinormal modes, Phys. Rev. D92, 124006 (2015)

  22. [22]

    Wang and C

    M. Wang and C. Herdeiro, Maxwell perturbations on Kerr–anti–de Sitter black holes: Quasinormal modes, su- perradiant instabilities, and vector clouds, Phys. Rev. D 93, 064066 (2016)

  23. [23]

    M. Wang, Z. Chen, Q. Pan, and J. Jing, Maxwell quasi- normal modes on a global monopole Schwarzschild-anti- de Sitter black hole with Robin boundary conditions, Eur. Phys. J. C81, 469 (2021)

  24. [24]

    M. Wang, Z. Chen, X. Tong, Q. Pan, and J. Jing, Bifur- cation of the Maxwell quasinormal spectrum on asymp- totically anti–de Sitter black holes, Phys. Rev. D103, 064079 (2021)

  25. [25]

    H. F. Liu and D. f. Zeng, Master functions of Reissner- Nordström black hole perturbations and their Darboux transformation, Phys. Rev. D112, 044025 (2025)

  26. [26]

    Regge and J

    T. Regge and J. A. Wheeler, Stability of a Schwarzschild singularity, Phys. Rev.108, 1063 (1957)

  27. [27]

    F. J. Zerilli, Effective potential for even parity Regge- Wheeler gravitational perturbation equations, Phys. Rev. Lett.24, 737 (1970)

  28. [28]

    F. J. Zerilli, Gravitational field of a particle falling in a schwarzschild geometry analyzed in tensor harmonics, Phys. Rev. D2, 2141 (1970)

  29. [29]

    F. J. Zerilli, Perturbation analysis for gravitational and electromagnetic radiation in a Reissner-Nordstroem ge- ometry, Phys. Rev. D9, 860 (1974)

  30. [30]

    S.JhinganandT.Tanaka, Improvementonthemetricre- construction scheme in Regge-Wheeler-Zerilli formalism, Phys. Rev. D67, 104018 (2003)

  31. [31]

    R. J. Gleiser, C. O. Nicasio, R. H. Price, and J. Pullin, Second order perturbations of a Schwarzschild black hole, Classical Quantum Gravity13, L117-L124 (1996)

  32. [32]

    R. J. Gleiser, C. O. Nicasio, R. H. Price, and J. Pullin, Gravitational radiation from Schwarzschild black holes: The Second order perturbation formalism, Phys. Rept. 325, 41-81 (2000)

  33. [33]

    Nakano and K

    H. Nakano and K. Ioka, Second-order quasinormal mode of the Schwarzschild black hole, Phys. Rev. D76, 084007 (2007)

  34. [34]

    Lenzi and C

    M. Lenzi and C. F. Sopuerta, Gauge-independent met- ric reconstruction of perturbations of vacuum spherically symmetric spacetimes, Phys. Rev. D109084030 (2024),

  35. [35]

    Loutrel, J

    N. Loutrel, J. L. Ripley, E. Giorgi, and F. Pretorius, Sec- ond order perturbations of kerr black holes: Reconstruc- tion of the first-order metric, Phys. Rev. D103, 104017 (2021),

  36. [36]

    Spiers, A

    A. Spiers, A. Pound, and J. Moxon, Second-order Teukol- sky formalism in Kerr spacetime: Formulation and non- linear source, Phys. Rev. D108, 064002 (2023),

  37. [37]

    Spiers, A

    A. Spiers, A. Pound, and B. Wardell, Second-order per- turbations of the Schwarzschild spacetime: Practical, co- variant, and gauge-invariant formalisms, Phys. Rev. D 110064030 (2024),

  38. [38]

    Brizuela, J

    D. Brizuela, J. M. Martin-Garcia, and G. A. Mena Maru- gan, Second and higher-order perturbations of a spherical spacetime, Phys. Rev. D74, 044039 (2006),

  39. [39]

    Moncrief, Odd-parity stability of a Reissner- Nordstrom black hole, Phys

    V. Moncrief, Odd-parity stability of a Reissner- Nordstrom black hole, Phys. Rev. D9, 2707 (1974)

  40. [40]

    Moncrief, Stability of Reissner-Nordstrom black holes, Phys

    V. Moncrief, Stability of Reissner-Nordstrom black holes, Phys. Rev. D10, 1057 (1974)

  41. [41]

    Lenzi and C

    M. Lenzi and C. F. Sopuerta, Master functions and equa- tions for perturbations of vacuum spherically symmetric spacetimes, Phys. Rev. D104, 084053 (2021),

  42. [42]

    Lenzi and C

    M. Lenzi and C. F. Sopuerta, Darboux covariance: A hidden symmetry of perturbed Schwarzschild black holes, Phys. Rev. D104, 124068 (2021),

  43. [43]

    Bruni, S

    M. Bruni, S. Matarrese, S. Mollerach, and S. Sonego, Perturbations of space-time: Gauge transformations and gauge invariance at second order and beyond, Classical Quantum Gravity14, 2585-2606 (1997)

  44. [44]

    R. G. Daghigh, M. D. Green, and J. C. Morey, Calculat- ing quasinormal modes of Schwarzschild anti–de Sitter black holes using the continued fraction method, Phys. Rev. D107, 024023 (2023)

  45. [45]

    M. Wang, C. Herdeiro, and J. Jing, Dirac perturbations on Schwarzschild–anti–de Sitter spacetimes: Generic boundary conditions and new quasinormal modes, Phys. Rev. D96, 104035 (2017)

  46. [46]

    M. Wang, C. Herdeiro, and J. Jing, Charged Dirac per- turbations on Reissner-Nordström–anti–de Sitter space- times: Quasinormal modes with Robin boundary condi- tions, Phys. Rev. D100, 124062 (2019)

  47. [47]

    L. N. Trefethen, Spectral methods in MATLAB (Siam, 2000)

  48. [48]

    Fortuna and I

    S. Fortuna and I. Vega, Electromagnetic quasinormal modes of Schwarzschild–anti–de Sitter black holes: Bi- furcations, spectral similarity, and exact solutions in the large black hole limit, Phys. Rev. D106, 084028 (2022)

  49. [49]

    I. G. Moss and J. P. Norman, Gravitational quasinormal modes for anti-de Sitter black holes, Classical Quantum Gravity19, 2323-2332 (2002)

  50. [50]

    A. K. W. Chung, P. Wagle, and N. Yunes, Spec- tral method for the gravitational perturbations of black 11 holes: Schwarzschild background case, Phys. Rev. D107, 124032 (2023)

  51. [51]

    A. K. W. Chung, P. Wagle, and N. Yunes, Spectral method for metric perturbations of black holes: Kerr background case in general relativity, Phys. Rev. D109, 044072 (2024)

  52. [52]

    A. K. W. Chung and N. Yunes, Ringing out general rel- ativity: Quasinormal mode frequencies for black holes of any spin in modified gravity, Phys. Rev. Lett.133, 181401 (2024)

  53. [53]

    A. K. W. Chung and N. Yunes, Quasinormal mode fre- quencies and gravitational perturbations of black holes with any subextremal spin in modified gravity through METRICS: The scalar-Gauss-Bonnet gravity case, Phys. Rev. D110, 064019 (2024)

  54. [54]

    A. K. W. Chung, K. K. H. Lam, and N. Yunes, Quasinor- mal mode frequencies and gravitational perturbations of spinning black holes in modified gravity through MET- RICS: The dynamical Chern-Simons gravity case, Phys. Rev. D111, 124052 (2025)

  55. [55]

    E. W. Leaver, An Analytic representation for the quasi normal modes of Kerr black holes, Proc. Roy. Soc. Lond. A402, 285-298 (1985)

  56. [56]

    H. P. Nollert, Quasinormal modes of Schwarzschild black holes: The determination of quasinormal frequencies with very large imaginary parts, Phys. Rev. D47, 5253- 5258 (1993)

  57. [57]

    W. Liu, X. Fang, J. Jing, and J. Wang, Gravito- electromagnetic perturbations of MOG black holes with a cosmological constant: Quasinormal modes and ring- down waveforms, J. Cosmol. Astropart. Phys.11, 057 (2023),

  58. [58]

    W. Liu, C. Wen, and J. Wang, Lorentz violation allevi- ates gravitationally induced entanglement degradation, JHEP01, 184 (2025)

  59. [59]

    J. Z. Liu, W. D. Guo, S. W. Wei, and Y. X. Liu, Charged spherically symmetric and slowly rotating charged black hole solutions in bumblebee gravity, Eur. Phys. J. C85, 145 (2025)

  60. [60]

    W. Deng, W. Liu, F. Long, K. Xiao, and J. Jing, Quasi- normal modes of a massive scalar field in slowly rotating Einstein-Bumblebee black holes, J. Cosmol. Astropart. Phys.11, 028 (2025)

  61. [61]

    B. R. Li, J. Z. Liu, W. D. Guo, and Y. X. Liu, Quasinor- mal modes of a charged spherically symmetric black hole in bumblebee gravity, arXiv:2510.20503

  62. [62]

    Casana, A

    R. Casana, A. Cavalcante, F. P. Poulis, and E. B. Santos, Exact Schwarzschild-like solution in a bumblebee gravity model, Phys. Rev. D97, 104001 (2018)

  63. [63]

    R. V. Maluf and J. C. S. Neves, Black holes with a cos- mological constant in bumblebee gravity, Phys. Rev. D 103, 044002 (2021)