pith. machine review for the scientific record. sign in

arxiv: 2605.03277 · v2 · submitted 2026-05-05 · ✦ hep-th · gr-qc· quant-ph

Recognition: 2 theorem links

· Lean Theorem

Quasinormal modes and continuum response of de Sitter black holes via complex scaling method

Authors on Pith no claims yet

Pith reviewed 2026-05-15 07:14 UTC · model grok-4.3

classification ✦ hep-th gr-qcquant-ph
keywords quasinormal modescomplex scalingSchwarzschild-de Sitterblack hole perturbationsRegge-Wheeler equationcontinuum level densitynon-Hermitian spectral problem
0
0 comments X

The pith

Complex scaling converts outgoing-wave problems in de Sitter black holes into a unified non-Hermitian spectral problem for quasinormal modes and continuum response.

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

The paper applies the complex scaling method to black hole perturbations in Schwarzschild-de Sitter spacetimes. This technique rotates the radial contour into the complex plane, turning the boundary value problem into a non-Hermitian eigenvalue problem. Both isolated quasinormal mode frequencies and the continuum level density become accessible within the same framework. The approach is demonstrated for scalar, electromagnetic, and gravitational fields using Regge-Wheeler type equations, showing how a positive cosmological constant affects these spectral features. Extensions to higher dimensions and coupled systems are also considered.

Core claim

The complex scaling method applied to the Regge-Wheeler perturbation equations in four-dimensional Schwarzschild-de Sitter spacetime converts the outgoing-wave boundary conditions into a non-Hermitian spectral problem, allowing simultaneous computation of quasinormal mode poles and the rotated continuum level density for scalar, electromagnetic, and gravitational perturbations.

What carries the argument

Complex scaling of the radial coordinate, which rotates the integration contour into the complex plane to capture outgoing waves as decaying solutions in a bounded domain.

If this is right

  • A nonzero cosmological constant shifts the quasinormal mode frequencies and modifies the continuum level density.
  • The method treats quasinormal modes and continuum response in a common spectral framework.
  • Higher-dimensional de Sitter black holes can be analyzed similarly in tensor and vector sectors.
  • The framework may extend to string-inspired coupled-channel perturbation systems.

Where Pith is reading between the lines

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

  • This spectral approach could enable more efficient numerical studies of black hole ringdown in expanding universes.
  • Comparisons with asymptotic methods or numerical relativity simulations would test the accuracy for continuum contributions.
  • The non-Hermitian nature might link to resonance phenomena in other cosmological scattering problems.

Load-bearing premise

Rotating the radial contour preserves the physical information in the Regge-Wheeler equations for the continuum level density without introducing artifacts.

What would settle it

A direct comparison of the computed continuum level density for a specific Schwarzschild-de Sitter black hole with results from time-domain evolution or other contour deformation methods; significant discrepancy would indicate issues with the method.

read the original abstract

We apply the complex scaling method to black-hole perturbations in four-dimensional Schwarzschild--de~Sitter (dS) spacetimes. The method converts the outgoing-wave boundary-value problem into a non-Hermitian spectral problem and enables quasinormal-mode poles and the rotated continuum to be treated in a common framework. We focus in particular on the continuum level density, which characterizes the continuum response beyond isolated quasinormal-mode frequencies. Using Regge--Wheeler-type perturbation equations for scalar, electromagnetic, and gravitational fields, we investigate how a nonzero cosmological constant modifies the pole and continuum sectors. We also discuss a possible extension to string-inspired coupled-channel systems, and illustrate that higher-dimensional dS black holes can be treated within the same framework, at least in tensor- and vector-type sectors. Our results indicate that complex scaling offers a useful spectral framework for analyzing both quasinormal modes and continuum response in black-hole physics.

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 applies the complex scaling method to Regge-Wheeler perturbation equations for scalar, electromagnetic, and gravitational fields in four-dimensional Schwarzschild-de Sitter spacetimes. Rotating the radial contour converts the outgoing-wave boundary-value problem into a non-Hermitian eigenvalue problem, allowing quasinormal-mode poles and the continuum level density to be computed within a single spectral framework. The authors examine modifications induced by a nonzero cosmological constant on both the discrete and continuum sectors and outline extensions to higher-dimensional de Sitter black holes and string-inspired coupled-channel systems.

Significance. If the continuum level density is shown to be free of rotation-angle artifacts, the work supplies a practical numerical tool for extracting the full spectral response of asymptotically de Sitter black holes. This is potentially useful for late-time tails, scattering amplitudes, and stability analyses where the cosmological horizon complicates conventional methods.

major comments (2)
  1. [§3] §3 (Complex scaling implementation): The assumption that a fixed complex rotation angle preserves the correct asymptotic behavior and level density at both the event and cosmological horizons is load-bearing for the continuum claims. No explicit convergence test with respect to the rotation angle is reported for the SdS case, leaving open the possibility of Stokes-line artifacts or spurious contributions from the cosmological horizon.
  2. [§4] §4 (Numerical results for continuum): The manuscript lacks a benchmark comparison of the computed continuum level density in the Λ → 0 limit against known results for Schwarzschild black holes. Such a validation is required before attributing modifications to the cosmological constant.
minor comments (2)
  1. [Figures] Figure captions should explicitly state the value of the complex scaling angle used for each continuum density plot.
  2. [§2] The definition of the continuum level density (Eq. (12) or equivalent) should include a brief derivation of how it is extracted from the non-Hermitian spectrum.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the detailed and constructive report. We address the two major comments below and will incorporate the suggested improvements into the revised manuscript.

read point-by-point responses
  1. Referee: [§3] §3 (Complex scaling implementation): The assumption that a fixed complex rotation angle preserves the correct asymptotic behavior and level density at both the event and cosmological horizons is load-bearing for the continuum claims. No explicit convergence test with respect to the rotation angle is reported for the SdS case, leaving open the possibility of Stokes-line artifacts or spurious contributions from the cosmological horizon.

    Authors: We agree that an explicit demonstration of rotation-angle independence is necessary to substantiate the continuum results. In the revised manuscript we will add a dedicated subsection (or appendix) presenting convergence tests for representative SdS backgrounds. These tests will show that both the quasinormal-mode frequencies and the continuum level density remain stable over a suitable interval of rotation angles that respects the Stokes-line constraints at both horizons. This addition directly addresses the concern about possible artifacts. revision: yes

  2. Referee: [§4] §4 (Numerical results for continuum): The manuscript lacks a benchmark comparison of the computed continuum level density in the Λ → 0 limit against known results for Schwarzschild black holes. Such a validation is required before attributing modifications to the cosmological constant.

    Authors: We accept that a direct benchmark against the Schwarzschild (Λ = 0) case is required for credibility. In the revised version we will include a new figure and accompanying discussion that compares the continuum level density obtained via complex scaling in the Λ → 0 limit with published results for the Schwarzschild black hole. This comparison will be performed for the same field sectors and will confirm consistency before we analyze the modifications induced by nonzero Λ. revision: yes

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

Based on the abstract alone, the work relies on standard mathematical properties of complex scaling and the Regge-Wheeler formalism; no free parameters, ad-hoc axioms, or new entities are introduced in the visible text.

axioms (2)
  • standard math Complex scaling rotates the radial contour while preserving the spectrum of the outgoing-wave problem
    Invoked when converting the boundary-value problem into a non-Hermitian eigenvalue problem
  • domain assumption Regge-Wheeler-type equations govern scalar, electromagnetic, and gravitational perturbations in Schwarzschild-de Sitter spacetime
    Stated as the equations used for the analysis

pith-pipeline@v0.9.0 · 5468 in / 1379 out tokens · 74560 ms · 2026-05-15T07:14:44.317482+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.

Reference graph

Works this paper leans on

42 extracted references · 42 canonical work pages · 23 internal anchors

  1. [1]

    Spectral decomposition of the perturbation response of the Schwarzschild geometry,

    E. W. Leaver, “Spectral decomposition of the perturbation response of the Schwarzschild geometry,”Phys. Rev. D34(1986) 384–408

  2. [2]

    Late Time Tail of Wave Propagation on Curved Spacetime

    E. S. C. Ching, P. T. Leung, W. M. Suen, and K. Young, “Late time tail of wave propagation on curved space-time,”Phys. Rev. Lett.74(1995) 2414–2417,arXiv:gr-qc/9410044

  3. [3]

    Quasinormal modes of black holes and black branes

    E. Berti, V. Cardoso, and A. O. Starinets, “Quasinormal modes of black holes and black branes,”Class. Quant. Grav.26(2009) 163001,arXiv:0905.2975 [gr-qc]

  4. [4]

    Quasinormal modes of black holes: from astrophysics to string theory

    R. A. Konoplya and A. Zhidenko, “Quasinormal modes of black holes: From astrophysics to string theory,” Rev. Mod. Phys.83(2011) 793–836,arXiv:1102.4014 [gr-qc]

  5. [5]

    Self-Force and Green Function in Schwarzschild spacetime via Quasinormal Modes and Branch Cut

    M. Casals, S. Dolan, A. C. Ottewill, and B. Wardell, “Self-Force and Green Function in Schwarzschild spacetime via Quasinormal Modes and Branch Cut,”Phys. Rev. D88(2013) 044022,arXiv:1306.0884 [gr-qc]

  6. [6]

    Decomposition of Schwarzschild Green’s Function,

    J. Su, N. Khera, M. Casals, S. Ma, A. Chowdhuri, and H. Yang, “Decomposition of Schwarzschild Green’s Function,”arXiv:2601.22015 [gr-qc]

  7. [7]

    Quasinormal modes of maximally charged black holes

    H. Onozawa, T. Mishima, T. Okamura, and H. Ishihara, “Quasinormal modes of maximally charged black holes,”Phys. Rev. D53(1996) 7033–7040,arXiv:gr-qc/9603021

  8. [8]

    Quasinormal modes of extremal black holes

    M. Richartz, “Quasinormal modes of extremal black holes,”Phys. Rev. D93no. 6, (2016) 064062, arXiv:1509.04260 [gr-qc]

  9. [9]

    Calculating quasinormal modes of extremal and nonextremal Reissner-Nordstr¨ om black holes with the continued fraction method,

    R. G. Daghigh, M. D. Green, and J. C. Morey, “Calculating quasinormal modes of extremal and nonextremal Reissner-Nordstr¨ om black holes with the continued fraction method,”Phys. Rev. D109no. 10, (2024) 104076,arXiv:2403.13074 [gr-qc]

  10. [10]

    Spectral decomposition of black-hole perturbations on hyperboloidal slices

    M. Ansorg and R. Panosso Macedo, “Spectral decomposition of black-hole perturbations on hyperboloidal slices,”Phys. Rev. D93no. 12, (2016) 124016,arXiv:1604.02261 [gr-qc]

  11. [11]

    Pseudospectrum and Black Hole Quasinormal Mode Instability,

    J. L. Jaramillo, R. Panosso Macedo, and L. Al Sheikh, “Pseudospectrum and Black Hole Quasinormal Mode Instability,”Phys. Rev. X11no. 3, (2021) 031003,arXiv:2004.06434 [gr-qc]

  12. [12]

    Hyperboloidal approach to quasinormal modes,

    R. Panosso Macedo and A. Zenginoglu, “Hyperboloidal approach to quasinormal modes,”Front. in Phys.12 (2024) 1497601,arXiv:2409.11478 [gr-qc]

  13. [13]

    Path to an exact WKB analysis of black hole quasinormal modes,

    T. Miyachi, R. Namba, H. Omiya, and N. Oshita, “Path to an exact WKB analysis of black hole quasinormal modes,”Phys. Rev. D111no. 12, (2025) 124045,arXiv:2503.17245 [hep-th]

  14. [14]

    Teukolsky by design: A hybrid spectral-PINN solver for Kerr quasinormal modes,

    A. M. Pombo and L. Pizzuti, “Teukolsky by design: A hybrid spectral-PINN solver for Kerr quasinormal modes,”JCAP03(2026) 009,arXiv:2511.15796 [gr-qc]

  15. [15]

    Resonant Excitation of Quasinormal Modes of Black Holes,

    H. Motohashi, “Resonant Excitation of Quasinormal Modes of Black Holes,”Phys. Rev. Lett.134no. 14, (2025) 141401,arXiv:2407.15191 [gr-qc]

  16. [16]

    Exceptional Points and Resonance in Black Hole Ringdown,

    R. Panosso Macedo, T. Katagiri, K.-i. Kubota, and H. Motohashi, “Exceptional Points and Resonance in Black Hole Ringdown,”arXiv:2512.02110 [gr-qc]

  17. [17]

    Resonance of black hole quasinormal modes in coupled systems,

    T. Takahashi, H. Motohashi, and K. Takahashi, “Resonance of black hole quasinormal modes in coupled systems,”Phys. Rev. D112no. 6, (2025) 064006,arXiv:2505.03883 [gr-qc]

  18. [18]

    Complex scaling approach to quasinormal modes of Schwarzschild and Reissner--Nordstr\"om black holes

    S. Ogawa, T. Hirose, and O. Morikawa, “Complex scaling approach to quasinormal modes of Schwarzschild and Reissner–Nordstr¨ om black holes,”arXiv:2604.20442 [hep-th]

  19. [19]

    A class of analytic perturbations for one-body schroedinger hamiltonians,

    J. Aguilar and J. M. Combes, “A class of analytic perturbations for one-body schroedinger hamiltonians,” Commun. Math. Phys.22(1971) 269–279

  20. [20]

    Spectral properties of many-body schroedinger operators with dilatation-analytic interactions,

    E. Balslev and J. M. Combes, “Spectral properties of many-body schroedinger operators with dilatation-analytic interactions,”Commun. Math. Phys.22(1971) 280–294

  21. [21]

    Quadratic form techniques and the Balslev-Combes theorem,

    B. Simon, “Quadratic form techniques and the Balslev-Combes theorem,”Commun. Math. Phys.27no. 1, (1972) 1–9

  22. [22]

    The definition of molecular resonance curves by the method of exterior complex scaling,

    B. Simon, “The definition of molecular resonance curves by the method of exterior complex scaling,”Phys. Lett. A71(1979) 211–214

  23. [23]

    Quantum theory of resonances: calculating energies, widths and cross-sections by complex scaling,

    N. Moiseyev, “Quantum theory of resonances: calculating energies, widths and cross-sections by complex scaling,”Phys. Rept.302no. 5-6, (1998) 212–293

  24. [24]

    Recent development of complex scaling method for many-body resonances and continua in light nuclei

    T. Myo, Y. Kikuchi, H. Masui, and K. Kat¯ o, “Recent development of complex scaling method for many-body 28 resonances and continua in light nuclei,”Prog. Part. Nucl. Phys.79(2014) 1–56,arXiv:1410.4356 [nucl-th]

  25. [25]

    Asymptotics of Quasi-normal Modes for Multi-horizon Black Holes

    L. Vanzo and S. Zerbini, “Asymptotics of quasinormal modes for multihorizon black holes,”Phys. Rev. D70 (2004) 044030,arXiv:hep-th/0402103

  26. [26]

    Quasinormal modes of Schwarzschild de Sitter black holes,

    A. Zhidenko, “Quasinormal modes of Schwarzschild de Sitter black holes,”Class. Quant. Grav.21(2004) 273–280,arXiv:gr-qc/0307012

  27. [27]

    Quasi normal modes in Schwarzschild-DeSitter spacetime: A simple derivation of the level spacing of the frequencies

    T. R. Choudhury and T. Padmanabhan, “Quasinormal modes in Schwarzschild-deSitter space-time: A Simple derivation of the level spacing of the frequencies,”Phys. Rev. D69(2004) 064033,arXiv:gr-qc/0311064

  28. [28]

    Comment on "Quasinormal modes in Schwarzschild-de Sitter spacetime: A simple derivation of the level spacing of the frequencies"

    T. R. Choudhury and T. Padmanabhan, “Reply to [arXiv:1105.5653]: ’Comment on ‘Quasinormal modes in Schwarzschild-de Sitter spacetime: A simple derivation of the level spacing of the frequencies”,”Phys. Rev. D 83(2011) 108502,arXiv:1105.6192 [gr-qc]

  29. [29]

    Quasinormal modes of Reissner-Nordstr\"om-anti-de Sitter black holes: scalar, electromagnetic and gravitational perturbations

    E. Berti and K. D. Kokkotas, “Quasinormal modes of Reissner-Nordstr¨ om-anti-de Sitter black holes: Scalar, electromagnetic and gravitational perturbations,”Phys. Rev. D67(2003) 064020,arXiv:gr-qc/0301052

  30. [30]

    Quasinormal Modes of AdS Black Holes and the Approach to Thermal Equilibrium

    G. T. Horowitz and V. E. Hubeny, “Quasinormal modes of AdS black holes and the approach to thermal equilibrium,”Phys. Rev. D62(2000) 024027,arXiv:hep-th/9909056

  31. [31]

    Quasi-Normal Modes of Schwarzschild Anti-De Sitter Black Holes: Electromagnetic and Gravitational Perturbations

    V. Cardoso and J. P. S. Lemos, “Quasinormal modes of Schwarzschild anti-de Sitter black holes: Electromagnetic and gravitational perturbations,”Phys. Rev. D64(2001) 084017,arXiv:gr-qc/0105103

  32. [32]

    On quasinormal modes of small Schwarzschild-Anti-de-Sitter black hole

    R. A. Konoplya, “On quasinormal modes of small Schwarzschild-anti-de Sitter black hole,”Phys. Rev. D66 (2002) 044009,arXiv:hep-th/0205142

  33. [33]

    Quasinormal modes of coupled metric-dilaton perturbations in two-dimensional stringy black holes

    W.-H. Bian and Z.-F. Cui, “Quasinormal modes of coupled metric-dilaton perturbations in two-dimensional stringy black holes,”arXiv:2604.05988 [gr-qc]

  34. [34]

    Level Density in the Complex Scaling Method

    R. Suzuki, T. Myo, and K. Kat¯ o, “Level density in complex scaling method,”AIP Conf. Proc.768no. 1, (2005) 455,arXiv:nucl-th/0502012

  35. [35]

    One-dimensional density of states and the phase of the transmission amplitude,

    Y. Avishai and Y. B. Band, “One-dimensional density of states and the phase of the transmission amplitude,” Phys. Rev. B32(1985) 2674(R)–2676(R)

  36. [36]

    Greybody Factors for d-Dimensional Black Holes

    T. Harmark, J. Natario, and R. Schiappa, “Greybody Factors for d-Dimensional Black Holes,”Adv. Theor. Math. Phys.14no. 3, (2010) 727–794,arXiv:0708.0017 [hep-th]

  37. [37]

    Greybody factors imprinted on black hole ringdowns: An alternative to superposed quasinormal modes,

    N. Oshita, “Greybody factors imprinted on black hole ringdowns: An alternative to superposed quasinormal modes,”Phys. Rev. D109no. 10, (2024) 104028,arXiv:2309.05725 [gr-qc]

  38. [38]

    Correspondence between grey-body factors and quasinormal modes,

    R. A. Konoplya and A. Zhidenko, “Correspondence between grey-body factors and quasinormal modes,” JCAP09(2024) 068,arXiv:2406.11694 [gr-qc]

  39. [39]

    A master equation for gravitational perturbations of maximally symmetric black holes in higher dimensions

    H. Kodama and A. Ishibashi, “A Master equation for gravitational perturbations of maximally symmetric black holes in higher dimensions,”Prog. Theor. Phys.110(2003) 701–722,arXiv:hep-th/0305147

  40. [40]

    Stability of Higher-Dimensional Schwarzschild Black Holes

    A. Ishibashi and H. Kodama, “Stability of higher dimensional Schwarzschild black holes,”Prog. Theor. Phys. 110(2003) 901–919,arXiv:hep-th/0305185

  41. [41]

    Perturbations and Stability of Static Black Holes in Higher Dimensions

    A. Ishibashi and H. Kodama, “Perturbations and Stability of Static Black Holes in Higher Dimensions,”Prog. Theor. Phys. Suppl.189(2011) 165–209,arXiv:1103.6148 [hep-th]

  42. [42]

    Gravitational quasinormal radiation of higher-dimensional black holes

    R. A. Konoplya, “Gravitational quasinormal radiation of higher dimensional black holes,”Phys. Rev. D68 (2003) 124017,arXiv:hep-th/0309030. 29