pith. machine review for the scientific record. sign in

arxiv: 2604.27980 · v1 · submitted 2026-04-30 · 🌀 gr-qc · hep-th

Recognition: unknown

On mass inflation and thin shells in quasi-topological gravity

Authors on Pith no claims yet

Pith reviewed 2026-05-07 06:39 UTC · model grok-4.3

classification 🌀 gr-qc hep-th
keywords quasi-topological gravityregular black holesmass inflationnull thin shellsjunction conditionsinner horizon stabilitydistributional theorymodified gravity
0
0 comments X

The pith

Regular black holes in quasi-topological gravity admit no null thin shells under standard junction conditions.

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

The paper examines how null junction conditions work in re-summed quasi-topological gravity. It concludes that the pure-gravity regular black hole solutions in these theories do not permit null thin shells according to ordinary distributional rules. Without those shells the familiar thin-shell argument for mass inflation at the inner horizon cannot be applied. The stability of those inner horizons therefore remains unsettled and needs examination by methods that avoid thin shells and the vacuum restriction.

Core claim

We study the null junction conditions in (re-summed) quasi-topological gravity theories, showing that no null thin shells exist within the realms of standard distributional theory for the pure gravity regular black hole solutions we have analyzed. This implies that the usual derivation of the mass inflation instability, which makes use of null thin shells, is not applicable in these theories. The problem of stability of inner horizons of regular black holes in quasi-topological gravity is hence still open and must be addressed with a more refined analysis, which does not rely on thin shells or the vacuum condition.

What carries the argument

Null junction conditions adapted to quasi-topological gravity, which rule out null thin shells in the vacuum regular black hole spacetimes.

If this is right

  • The thin-shell derivation of mass inflation instability does not apply to these regular black hole solutions.
  • Inner-horizon stability in quasi-topological gravity cannot be settled by the usual mass-inflation argument.
  • Any stability analysis must employ techniques that do not invoke thin shells or the vacuum condition.
  • The same absence of null shells may appear in other higher-curvature regular black hole models.

Where Pith is reading between the lines

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

  • Numerical or perturbative methods will be needed to check whether inner horizons remain stable without relying on thin shells.
  • Regular black holes in these theories might evade the classical mass-inflation instability found in general relativity.
  • Non-vacuum or rotating extensions could be examined to see if null shells become possible once matter fields are added.

Load-bearing premise

The distributional junction conditions of general relativity transfer directly to quasi-topological gravity and the solutions under study are pure vacuum configurations.

What would settle it

A calculation that produces a nonzero surface stress-energy tensor on a null hypersurface while satisfying both the quasi-topological field equations and one of the regular black hole metrics would show that null thin shells can exist.

Figures

Figures reproduced from arXiv: 2604.27980 by Aravindhan Srinivasan, David Kubiznak, Francesco Di Filippo.

Figure 1
Figure 1. Figure 1: FIG. 1: A pair of spherical null shells crossing at view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2 view at source ↗
read the original abstract

We study the null junction conditions in (re-summed) quasi-topological gravity theories, showing that no null thin shells exist within the realms of standard distributional theory for the pure gravity regular black hole solutions we have analyzed. This implies that the usual derivation of the mass inflation instability, which makes use of null thin shells, is not applicable in these theories. The problem of stability of inner horizons of regular black holes in quasi-topological gravity is hence still open and must be addressed with a more refined analysis, which does not rely on thin shells or the vacuum condition.

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

0 major / 3 minor

Summary. The manuscript derives the null junction conditions directly within re-summed quasi-topological gravity and applies them to the pure-gravity regular black hole solutions under consideration. It obtains a no-go result: no non-trivial null thin shells exist in the standard distributional sense. Consequently the conventional thin-shell argument for mass inflation does not apply, and the inner-horizon stability question is left open, requiring analysis that goes beyond thin shells or the vacuum assumption.

Significance. If the central no-go result holds, the work is significant because it demonstrates that the mass-inflation instability mechanism familiar from general relativity cannot be imported unchanged into quasi-topological gravity; the inner-horizon stability problem must be re-examined with theory-specific tools. The paper correctly limits its claim to the solutions examined and explicitly flags the need for further methods, thereby providing a clear, falsifiable boundary on the applicability of the thin-shell approach.

minor comments (3)
  1. [Abstract] The abstract and introduction would benefit from a brief, explicit statement of which specific regular black hole metrics (e.g., the exact form of f(r) or the re-summation parameter) were inserted into the junction conditions; this would make the scope of the no-go result immediately transparent to readers.
  2. In the section presenting the null junction conditions, the paper should display the explicit algebraic conditions on the metric functions (or their jumps) that lead to the vanishing of the surface stress-energy; without these intermediate expressions the verification of the no-go result remains opaque.
  3. A short paragraph comparing the derived junction conditions with the corresponding general-relativity expressions would help readers see precisely where the quasi-topological terms enforce the no-shell constraint.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their careful reading and positive assessment of our manuscript. The referee accurately captures our central no-go result on the absence of non-trivial null thin shells in the standard distributional sense for the pure-gravity regular black hole solutions in re-summed quasi-topological gravity, and correctly notes that this precludes the usual thin-shell derivation of mass inflation while leaving inner-horizon stability open for further study. We appreciate the referee's recognition that our claims are appropriately limited and that the work provides a clear boundary on the applicability of the thin-shell approach. Given the recommendation for minor revision and the lack of any specific comments requiring changes, we see no need for revisions at this stage.

Circularity Check

0 steps flagged

No significant circularity; direct no-go from junction conditions

full rationale

The paper's central result is obtained by deriving and applying the null junction conditions specific to (re-summed) quasi-topological gravity directly to the given pure-gravity regular black hole metrics. This produces the explicit no-go statement that no non-trivial null thin shells exist under standard distributional matching. The absence of thin shells then logically precludes the usual thin-shell-based mass-inflation argument, without any parameter fitting, redefinition of inputs as outputs, or load-bearing reliance on self-citations for the core calculation. The solutions themselves are treated as given inputs; the junction analysis is performed anew in the present theory rather than imported unchanged from GR. The paper explicitly bounds its conclusion to the examined cases and leaves inner-horizon stability open for non-vacuum or non-thin-shell methods. No step in the reported chain reduces by construction to its own inputs.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claim rests on the applicability of standard null junction conditions to quasi-topological gravity and on the vacuum character of the regular black hole solutions; no free parameters or invented entities are introduced in the abstract.

axioms (2)
  • domain assumption Standard distributional null junction conditions from general relativity apply without modification to quasi-topological gravity
    Invoked to conclude that no thin shells exist for the given solutions.
  • domain assumption The regular black hole solutions under study are pure gravity (vacuum) configurations
    The abstract specifies 'pure gravity regular black hole solutions' as the setting where shells are absent.

pith-pipeline@v0.9.0 · 5388 in / 1460 out tokens · 46484 ms · 2026-05-07T06:39:48.419676+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

59 extracted references · 37 canonical work pages · 1 internal anchor

  1. [1]

    for a discussion on the existence of thin shells in generic theories of gravity). In an attempt to allow for the existence of thin null shells, we relax the continuity ofG 3 and adopt one of the following two prescriptions to handle Θδterms: 5 5 A rigorous treatment of such products requires the use of gen- eralized (Colombeau) distributions [41–44], whic...

  2. [2]

    In the equations of motion, we first apply the rules (47), (48) and then use Θ(τ)δ(τ) = 1 2 δ(τ).(63)

  3. [3]

    As a second alternative, when evaluating the equa- tions of motion, we retain the powers of Θ Θn(τ),Θ n(−τ) = [1−Θ(τ)] n , Θj(τ)Θ k(−τ) = Θ j(τ)[1−Θ(τ)] k ,(64) and invoke the following rule: Θn(τ)δ(τ) = 1 n+ 1 δ(τ).(65) In both prescriptions, we deduce the following distri- butional form of the generalized Einstein tensorE ab: Eµν =E+ µνΘ(τ) +E − µνΘ(−τ)...

  4. [4]

    Poisson and W

    E. Poisson and W. Israel, Internal structure of black holes, Phys. Rev. D41, 1796 (1990)

  5. [5]

    Ori, Inner structure of a charged black hole: An exact mass-inflation solution, Phys

    A. Ori, Inner structure of a charged black hole: An exact mass-inflation solution, Phys. Rev. Lett.67, 789 (1991)

  6. [6]

    Carballo-Rubio, F

    R. Carballo-Rubio, F. Di Filippo, S. Liberati, C. Pacilio, and M. Visser, On the viability of regular black holes, JHEP07, 023, arXiv:1805.02675 [gr-qc]

  7. [7]

    Carballo-Rubio, F

    R. Carballo-Rubio, F. Di Filippo, S. Liberati, C. Pa- cilio, and M. Visser, Inner horizon instability and the unstable cores of regular black holes, JHEP05, 132, arXiv:2101.05006 [gr-qc]

  8. [8]

    Carballo-Rubio, F

    R. Carballo-Rubio, F. Di Filippo, S. Liberati, and M. Visser, Mass Inflation without Cauchy Horizons, Phys. Rev. Lett.133, 181402 (2024), arXiv:2402.14913 [gr-qc]

  9. [9]

    Di Filippo, R

    F. Di Filippo, R. Carballo-Rubio, S. Liberati, C. Pa- cilio, and M. Visser, On the Inner Horizon Instability of Non-Singular Black Holes, Universe8, 204 (2022), arXiv:2203.14516 [gr-qc]

  10. [10]

    Carballo-Rubio, F

    R. Carballo-Rubio, F. Di Filippo, S. Liberati, C. Pacilio, and M. Visser, Regular black holes without mass inflation instability, JHEP09, 118, arXiv:2205.13556 [gr-qc]

  11. [11]

    Bueno, P

    P. Bueno, P. A. Cano, and R. A. Hennigar, (Generalized) quasi-topological gravities at all orders, Class. Quant. Grav.37, 015002 (2020), arXiv:1909.07983 [hep-th]

  12. [12]

    Bueno, P

    P. Bueno, P. A. Cano, and R. A. Hennigar, Regular black holes from pure gravity, Phys. Lett. B861, 139260 (2025), arXiv:2403.04827 [gr-qc]

  13. [13]

    Bueno, P

    P. Bueno, P. A. Cano, R. A. Hennigar, and ´A. J. Murcia, Dynamical Formation of Regular Black Holes, Phys. Rev. Lett.134, 181401 (2025), arXiv:2412.02742 [gr-qc]

  14. [14]

    Bueno, P

    P. Bueno, P. A. Cano, R. A. Hennigar, and ´A. J. Murcia, Regular black holes from thin-shell collapse, Phys. Rev. D111, 104009 (2025), arXiv:2412.02740 [gr-qc]

  15. [15]

    V. P. Frolov and A. Zelnikov, Regular black holes in quasitopological gravity: Null shells and mass inflation, Phys. Rev. D113, 084007 (2026), arXiv:2601.01861 [gr- qc]

  16. [16]

    Lovelock, The Einstein tensor and its generalizations, J

    D. Lovelock, The Einstein tensor and its generalizations, J. Math. Phys.12, 498 (1971)

  17. [17]

    Dadhich, S

    N. Dadhich, S. G. Ghosh, and S. Jhingan, The Lovelock gravity in the critical spacetime dimension, Phys. Lett. B711, 196 (2012), arXiv:1202.4575 [gr-qc]

  18. [18]

    Gannouji, Y

    R. Gannouji, Y. Rodr´ ıguez Baez, and N. Dadhich, Pure Lovelock black holes in dimensionsd= 3N+1 are stable, Phys. Rev. D100, 084011 (2019), arXiv:1907.09503 [gr- qc]

  19. [19]

    Barrab` es, W

    C. Barrab` es, W. Israel, and E. Poisson, Collision of light- like shells and mass inflation in rotating black holes, Clas- sical and Quantum Gravity7, L273 (1990)

  20. [20]

    Barrabes and W

    C. Barrabes and W. Israel, Thin shells in general rela- tivity and cosmology: The Lightlike limit, Phys. Rev. D 43, 1129 (1991). 8 We see this explicitly for the null shells in each example by sub- stituting the conditions (A1) and (A3), together with the corre- sponding expressions for the Misner–Sharp mass, into (85). It is straightforward to verify the...

  21. [21]

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

  22. [22]

    S. A. Hayward, Formation and evaporation of regular black holes, Phys. Rev. Lett.96, 031103 (2006), arXiv:gr- qc/0506126

  23. [23]

    Poisson, A relativist’s toolkit: the mathematics of black-hole mechanics, Cambridge University Press (2004)

    E. Poisson, A relativist’s toolkit: the mathematics of black-hole mechanics, Cambridge University Press (2004)

  24. [24]

    Dray and G

    T. Dray and G. ’t Hooft, The Effect of Spherical Shells of Matter on the Schwarzschild Black Hole, Commun. Math. Phys.99, 613 (1985)

  25. [25]

    I. H. Redmount, Blue-Sheet Instability of Schwarzschild Wormholes, Progress of Theoretical Physics73, 1401 (1985)

  26. [26]

    C. W. Misner and D. H. Sharp, Relativistic equations for adiabatic, spherically symmetric gravitational collapse, Phys. Rev.136, B571 (1964)

  27. [27]

    W. C. Hernandez and C. W. Misner, Observer Time as a Coordinate in Relativistic Spherical Hydrodynamics, Astrophys. J.143, 452 (1966)

  28. [28]

    Maeda, Final fate of spherically symmetric gravita- tional collapse of a dust cloud in Einstein-Gauss-Bonnet gravity, Phys

    H. Maeda, Final fate of spherically symmetric gravita- tional collapse of a dust cloud in Einstein-Gauss-Bonnet gravity, Phys. Rev. D73, 104004 (2006), arXiv:gr- qc/0602109

  29. [29]

    Maeda and M

    H. Maeda and M. Nozawa, Generalized Misner-Sharp quasi-local mass in Einstein-Gauss-Bonnet gravity, Phys. Rev. D77, 064031 (2008), arXiv:0709.1199 [hep-th]

  30. [30]

    Cai, L.-M

    R.-G. Cai, L.-M. Cao, Y.-P. Hu, and N. Ohta, General- ized Misner-Sharp Energy in f(R) Gravity, Phys. Rev. D 80, 104016 (2009), arXiv:0910.2387 [hep-th]

  31. [31]

    Bueno, P

    P. Bueno, P. A. Cano, R. A. Hennigar, M. Lu, and J. Moreno, Generalized quasi-topological gravities: the whole shebang, Class. Quant. Grav.40, 015004 (2023), arXiv:2203.05589 [hep-th]

  32. [32]

    Moreno and ´A

    J. Moreno and ´A. J. Murcia, Classification of general- ized quasitopological gravities, Phys. Rev. D108, 044016 (2023), arXiv:2304.08510 [gr-qc]

  33. [33]

    Weyl, The theory of gravitation, Annalen Phys.54, 117 (1917)

    H. Weyl, The theory of gravitation, Annalen Phys.54, 117 (1917)

  34. [34]

    Lovelock, Spherically symmetric metrics and field equations in four-dimensional space, Il Nuovo Cimento B (1971-1996)14, 260 (1973)

    D. Lovelock, Spherically symmetric metrics and field equations in four-dimensional space, Il Nuovo Cimento B (1971-1996)14, 260 (1973)

  35. [35]

    Frausto, I

    G. Frausto, I. Kol´ aˇ r, T. M´ alek, and C. Torre, Symme- try reduction of gravitational Lagrangians, Phys. Rev. D 111, 064062 (2025), arXiv:2410.11036 [gr-qc]

  36. [36]

    Bueno, R

    P. Bueno, R. A. Hennigar, and ´A. J. Murcia, Birkhoff implies Quasi-topological, (2025), arXiv:2510.25823 [gr- qc]

  37. [37]

    Avil´ es, H

    L. Avil´ es, H. Maeda, and C. Martinez, Junction condi- tions in scalar–tensor theories, Class. Quant. Grav.37, 075022 (2020), arXiv:1910.07534 [gr-qc]

  38. [38]

    Padilla and V

    A. Padilla and V. Sivanesan, Boundary Terms and Junc- tion Conditions for Generalized Scalar-Tensor Theories, JHEP08, 122, arXiv:1206.1258 [gr-qc]

  39. [39]

    J. M. M. Senovilla, Junction conditions for F(R)-gravity and their consequences, Phys. Rev. D88, 064015 (2013), arXiv:1303.1408 [gr-qc]

  40. [40]

    Reina, J

    B. Reina, J. M. M. Senovilla, and R. Vera, Junction con- ditions in quadratic gravity: thin shells and double layers, 13 Class. Quant. Grav.33, 105008 (2016), arXiv:1510.05515 [gr-qc]

  41. [41]

    Mars and J

    M. Mars and J. M. M. Senovilla, Geometry of general hypersurfaces in space-time: Junction conditions, Class. Quant. Grav.10, 1865 (1993), arXiv:gr-qc/0201054

  42. [42]

    J. M. M. Senovilla, Equations for general shells, JHEP 11, 134, arXiv:1805.03582 [gr-qc]

  43. [43]

    J. M. M. Senovilla, Junction Conditions for General Gravitational Theories, (2026), arXiv:2603.04645 [gr-qc]

  44. [44]

    Colombeau, Elementary Introduction to New Gener- alized Functions, (1985)

    J. Colombeau, Elementary Introduction to New Gener- alized Functions, (1985)

  45. [45]

    Colombeau, Multiplication of Distributions: A Tool in Mathematics, Numerical Engineering and Theoretical Physics, Lecture Notes in Mathematics1532, 1 (1992)

    J.-F. Colombeau, Multiplication of Distributions: A Tool in Mathematics, Numerical Engineering and Theoretical Physics, Lecture Notes in Mathematics1532, 1 (1992)

  46. [46]

    Gsponer, A concise introduction to colombeau gener- alized functions and their applications in classical electro- dynamics, European Journal of Physics30, 109 (2009)

    A. Gsponer, A concise introduction to colombeau gener- alized functions and their applications in classical electro- dynamics, European Journal of Physics30, 109 (2009)

  47. [47]

    J. A. Silva, F. C. Carvalho, and A. R. G. Garcia, Gen- eralized junction conditions for discontinuous metrics, (2026), arXiv:2601.07936 [gr-qc]

  48. [48]

    D. G. Boulware and S. Deser, String Generated Gravity Models, Phys. Rev. Lett.55, 2656 (1985)

  49. [49]

    Hervik and M

    S. Hervik and M. Ortaggio, Universal Black Holes, JHEP 02, 047, arXiv:1907.08788 [gr-qc]

  50. [50]

    B. P. Dolan, A. Kostouki, D. Kubiznak, and R. B. Mann, Isolated critical point from Lovelock gravity, Class. Quant. Grav.31, 242001 (2014), arXiv:1407.4783 [hep-th]

  51. [51]

    R. A. Hennigar, D. Kubizˇ n´ ak, S. Murk, and I. Soranidis, Thermodynamics of regular black holes in anti-de Sitter space, JHEP11, 121, arXiv:2505.11623 [gr-qc]

  52. [52]

    Bardeen, Non-singular general relativistic gravita- tional collapse, Proceedings of the 5th International Con- ference on Gravitation and the Theory of Relativity , 87 (1968)

    J. Bardeen, Non-singular general relativistic gravita- tional collapse, Proceedings of the 5th International Con- ference on Gravitation and the Theory of Relativity , 87 (1968)

  53. [53]

    S. C. Davis, Generalized Israel junction conditions for a Gauss-Bonnet brane world, Phys. Rev. D67, 024030 (2003), arXiv:hep-th/0208205

  54. [54]

    Chu and H

    C.-S. Chu and H. S. Tan, Generalized Darmois–Israel Junction Conditions, Universe8, 250 (2022), arXiv:2103.06314 [hep-th]

  55. [55]

    Bueno, P

    P. Bueno, P. A. Cano, R. A. Hennigar, and ´A. J. Murcia, Regular black hole formation in four-dimensional non- polynomial gravities, Phys. Rev. D113, 024019 (2026), arXiv:2509.19016 [gr-qc]

  56. [56]

    Borissova and R

    J. Borissova and R. Carballo-Rubio, Regular black holes from pure gravity in four dimensions, (2026), arXiv:2602.16773 [gr-qc]

  57. [57]

    Cardoso, S

    V. Cardoso, S. Yoshida, O. J. C. Dias, and J. P. S. Lemos, Late time tails of wave propagation in higher dimensional space-times, Phys. Rev. D68, 061503 (2003), arXiv:hep- th/0307122

  58. [58]

    R. A. Konoplya and A. Zhidenko, Infinite tower of higher- curvature corrections: Quasinormal modes and late-time behavior of D-dimensional regular black holes, Phys. Rev. D109, 104005 (2024), arXiv:2403.07848 [gr-qc]

  59. [59]

    R. H. Price, Nonspherical perturbations of relativistic gravitational collapse. 1. Scalar and gravitational pertur- bations, Phys. Rev. D5, 2419 (1972)