pith. machine review for the scientific record. sign in

arxiv: 2604.18004 · v2 · submitted 2026-04-20 · ✦ hep-th · gr-qc

Recognition: unknown

Eikonal, nonlocality and regular black holes

Authors on Pith no claims yet

Pith reviewed 2026-05-10 04:48 UTC · model grok-4.3

classification ✦ hep-th gr-qc
keywords nonlocal gravityeikonal approximationregular black holesde Sitter coreSchwarzschild deformationasymptotically flat spacetimesscalar scattering
0
0 comments X

The pith

Nonlocal gravity yields singularity-free black holes with de Sitter cores through eikonal analysis.

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

The paper examines the leading gravitational eikonal in nonlocal D-dimensional gravity theories via tree-level 2 to 2 scalar scattering. It interprets the results as effective geometries: generalized Aichelburg-Sexl metrics for massless particles and smeared linearized Schwarzschild metrics for massive probes. These linearized solutions are then completed nonlinearly by imposing general conditions on the core behavior. The outcome is a class of asymptotically flat deformations of the Schwarzschild solution that remain regular everywhere and feature a de Sitter core. The authors also compute the main geometric and thermodynamic properties of the resulting spacetimes.

Core claim

In nonlocal D-dimensional gravity the eikonal limit of scalar scattering produces linearized geometries that, when completed nonlinearly using requirements on core behavior, become singularity-free asymptotically flat deformations of the Schwarzschild metric possessing a de Sitter core.

What carries the argument

Nonlinear completion of linearized eikonal geometries (generalized Aichelburg-Sexl for massless, smeared Schwarzschild for massive) guided by core-behavior requirements.

If this is right

  • The completed spacetimes contain no curvature singularities.
  • They remain asymptotically flat and approach the Schwarzschild metric at large distances.
  • Their interiors are described by a de Sitter geometry.
  • Geometric invariants and thermodynamic quantities such as temperature and entropy can be computed explicitly.
  • The construction applies to both massless and massive probe scattering in D dimensions.

Where Pith is reading between the lines

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

  • The de Sitter core sets a finite upper bound on curvature near the center.
  • Similar completions might be possible for other choices of nonlocal form factors.
  • Thermodynamic stability could be altered relative to classical Schwarzschild black holes because of the regular core.

Load-bearing premise

General requirements about the behavior of solutions in the core suffice to determine a unique nonlinear completion without an explicit derivation from the nonlocal action.

What would settle it

Direct solution of the nonlinear field equations from the underlying nonlocal action to check whether the proposed geometries satisfy them exactly.

read the original abstract

We investigate the leading gravitational eikonal in nonlocal $D$ dimensional theories of gravity. We analyze the simplest cases of $2\rightarrow2$ massless and massive scalar scattering at tree level, studying the effects of nonlocal form factors in the gravitational sector. We give an interpretation of our results in terms of geodesic motion in effective generalized Aichelburg-Sexl geometries for the massless case, and in smeared linearized Schwarzschild metrics for the massive case in the probe limit. Combining our results for the geometries at linearized level with general requirements about the behaviour of the solutions in the core, we propose a nonlinear completion of the geometries. The resulting spacetimes describe singularity-free, asymptotically flat deformations of the Schwarzschild solution with a de Sitter core. We also analyze the main geometric and thermodynamic features of these solutions.

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 computes the leading gravitational eikonal for tree-level 2→2 scattering of massless and massive scalars in nonlocal D-dimensional gravity theories. It interprets the results as effective linearized geometries: generalized Aichelburg-Sexl metrics for massless cases and smeared Schwarzschild metrics for massive cases in the probe limit. Using these linearized geometries combined with general requirements on the core behavior, the authors propose nonlinear completions that yield singularity-free, asymptotically flat black hole spacetimes with de Sitter cores, and analyze their geometric and thermodynamic properties.

Significance. The explicit tree-level eikonal calculations provide concrete, reproducible results on how nonlocal form factors modify effective geometries at linear order, which is a clear strength of the work. If the proposed nonlinear completions can be shown to satisfy the equations of motion from the nonlocal action, the paper would offer a useful route to constructing regular black holes in such theories. However, the heuristic character of the completion step means the strongest claims about singularity resolution remain provisional until further justification is supplied.

major comments (2)
  1. [§4] §4 (nonlinear completion): The proposal that the completed metrics are singularity-free deformations of Schwarzschild with de Sitter cores rests on 'general requirements about the behaviour of the solutions in the core' rather than an explicit derivation or verification that these metrics solve the integro-differential equations of motion implied by the nonlocal form factors beyond linear order. This step is load-bearing for the central claim in the abstract.
  2. [§3.2] §3.2 (massive case, probe limit): While the smeared linearized Schwarzschild metric is obtained from the eikonal amplitude, the subsequent nonlinear completion invokes external core requirements without demonstrating consistency with the underlying nonlocal action at quadratic or higher order in the metric perturbation.
minor comments (2)
  1. [§2] Notation for the nonlocal form factors (e.g., the precise definition of the exponential or entire function in the gravitational sector) should be stated explicitly in §2 to avoid ambiguity when comparing to prior literature on infinite-derivative gravity.
  2. [§5] The thermodynamic analysis in §5 would benefit from a direct comparison table of the Hawking temperature and entropy for the proposed metrics versus the standard Schwarzschild case at fixed mass.

Simulated Author's Rebuttal

2 responses · 1 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments. We address the major points below, clarifying the scope and limitations of our analysis while defending the approach taken in the paper.

read point-by-point responses
  1. Referee: [§4] §4 (nonlinear completion): The proposal that the completed metrics are singularity-free deformations of Schwarzschild with de Sitter cores rests on 'general requirements about the behaviour of the solutions in the core' rather than an explicit derivation or verification that these metrics solve the integro-differential equations of motion implied by the nonlocal form factors beyond linear order. This step is load-bearing for the central claim in the abstract.

    Authors: We agree that the nonlinear completions proposed in §4 are constructed by combining the linearized geometries obtained from the tree-level eikonal with general requirements on core regularity and asymptotic flatness, rather than by solving the full integro-differential equations of the nonlocal theory at nonlinear order. The manuscript explicitly frames this as a proposal ('we propose a nonlinear completion'), not a derivation from the complete action. This is a standard strategy when the nonlinear nonlocal equations are intractable, and the eikonal result supplies the physically motivated linear-order input. The abstract claim is limited to the proposal of such spacetimes, which we believe is accurately stated. We will revise §4 to more explicitly note the heuristic character and the provisional nature of the singularity-resolution claim. revision: partial

  2. Referee: [§3.2] §3.2 (massive case, probe limit): While the smeared linearized Schwarzschild metric is obtained from the eikonal amplitude, the subsequent nonlinear completion invokes external core requirements without demonstrating consistency with the underlying nonlocal action at quadratic or higher order in the metric perturbation.

    Authors: The nonlinear completion in the massive probe-limit case follows the same logic as in §4: the eikonal supplies the smeared linearized Schwarzschild geometry, which is then completed using the same general core requirements. We do not claim or demonstrate consistency at quadratic or higher order in the metric perturbation, as this would require solving the nonlocal equations beyond the leading eikonal approximation, which lies outside the scope of the present work. The probe limit and tree-level calculation are used precisely because they yield concrete, reproducible results at linear order. We will add a clarifying remark in §3.2 emphasizing these limitations. revision: partial

standing simulated objections not resolved
  • Explicit verification that the proposed nonlinear metrics satisfy the full integro-differential equations of motion from the nonlocal action at quadratic and higher orders.

Circularity Check

0 steps flagged

No significant circularity: linearized geometries from explicit amplitudes; nonlinear completion is a separate proposal

full rationale

The paper derives linearized geometries explicitly from tree-level eikonal scattering amplitudes in the nonlocal theory, interpreting them as generalized Aichelburg-Sexl metrics (massless case) and smeared Schwarzschild metrics (massive probe limit). The nonlinear completion is introduced separately by combining these results with external 'general requirements about the behaviour of the solutions in the core' to yield singularity-free asymptotically flat spacetimes with de Sitter cores. This step does not reduce any claimed prediction or first-principles result to the inputs by construction, nor does it rely on self-citation load-bearing, uniqueness theorems imported from the authors' prior work, or ansatzes smuggled via citation. The derivation chain is self-contained, with the scattering calculations providing independent content and the completion presented as a proposal rather than a forced or fitted outcome.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 1 invented entities

The paper assumes a standard nonlocal gravity setup with form factors and introduces a proposed nonlinear completion without independent evidence or derivation.

axioms (1)
  • domain assumption The leading gravitational eikonal can be extracted from tree-level 2-to-2 scalar scattering in nonlocal D-dimensional gravity
    Invoked as the starting point for both massless and massive cases.
invented entities (1)
  • Nonlinear completion of the linearized geometries no independent evidence
    purpose: To produce singularity-free spacetimes with de Sitter cores
    Proposed from linearized results plus general core requirements; no independent falsifiable handle given in abstract.

pith-pipeline@v0.9.0 · 5441 in / 1295 out tokens · 67401 ms · 2026-05-10T04:48:34.834283+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

107 extracted references · 89 canonical work pages · 1 internal anchor

  1. [1]

    Amati, M

    D. Amati, M. Ciafaloni and G. Veneziano,Superstring Collisions at Planckian Energies, Phys. Lett. B197(1987) 81

  2. [2]

    Amati, M

    D. Amati, M. Ciafaloni and G. Veneziano,Can Space-Time Be Probed Below the String Size?,Phys. Lett. B216(1989) 41

  3. [3]

    Amati, M

    D. Amati, M. Ciafaloni and G. Veneziano,Effective action and all order gravitational eikonal at Planckian energies,Nucl. Phys. B403(1993) 707. – 33 –

  4. [4]

    Verlinde and E

    H. Verlinde and E. Verlinde,Scattering at planckian energies,Nuclear Physics B371 (1992) 246–268

  5. [5]

    ’t Hooft,Graviton Dominance in Ultrahigh-Energy Scattering,Phys

    G. ’t Hooft,Graviton Dominance in Ultrahigh-Energy Scattering,Phys. Lett. B198(1987) 61

  6. [6]

    Muzinich and M

    I.J. Muzinich and M. Soldate,High-Energy Unitarity of Gravitation and Strings,Phys. Rev. D37(1988) 359

  7. [7]

    Di Vecchia, C

    P. Di Vecchia, C. Heissenberg, R. Russo and G. Veneziano,Universality of ultra-relativistic gravitational scattering,Phys. Lett. B811(2020) 135924 [2008.12743]

  8. [8]

    Koemans Collado, P

    A. Koemans Collado, P. Di Vecchia and R. Russo,Revisiting the second post-Minkowskian eikonal and the dynamics of binary black holes,Phys. Rev. D100(2019) 066028 [1904.02667]

  9. [9]

    Parra-Martinez, M.S

    J. Parra-Martinez, M.S. Ruf and M. Zeng,Extremal black hole scattering atO(G 3): graviton dominance, eikonal exponentiation, and differential equations,JHEP11(2020) 023 [2005.04236]

  10. [10]

    Accettulli Huber, A

    M. Accettulli Huber, A. Brandhuber, S. De Angelis and G. Travaglini,Eikonal phase matrix, deflection angle and time delay in effective field theories of gravity,Phys. Rev. D 102(2020) 046014 [2006.02375]

  11. [11]

    Di Vecchia, C

    P. Di Vecchia, C. Heissenberg, R. Russo and G. Veneziano,The eikonal approach to gravitational scattering and radiation atO(G 3),JHEP07(2021) 169 [2104.03256]. [12]LIGO Scientific, VIRGOcollaboration,GW150914: Observation of gravitational waves from a binary black hole merger,Nuovo Cim. C39(2017) 310. [13]LIGO Scientific, Virgocollaboration,GW170817: Obse...

  12. [12]

    Biswas, E

    T. Biswas, E. Gerwick, T. Koivisto and A. Mazumdar,Towards singularity and ghost free theories of gravity,Phys. Rev. Lett.108(2012) 031101 [1110.5249]

  13. [13]

    Modesto,Super-renormalizable quantum gravity,Phys

    L. Modesto,Super-renormalizable Quantum Gravity,Phys. Rev. D86(2012) 044005 [1107.2403]

  14. [14]

    Calcagni and L

    G. Calcagni and L. Modesto,Nonlocal quantum gravity and M-theory,Phys. Rev. D91 (2015) 124059 [1404.2137]

  15. [15]

    Bas i Beneito, G

    A. Bas i Beneito, G. Calcagni and L. Rachwal,Classical and quantum nonlocal gravity, in Handbook of Quantum Gravity, Springer Nature Singapore (2024), DOI [2211.05606]

  16. [16]

    Amati, M

    D. Amati, M. Ciafaloni and G. Veneziano,Classical and Quantum Gravity Effects from Planckian Energy Superstring Collisions,Int. J. Mod. Phys. A3(1988) 1615

  17. [17]

    Amati, M

    D. Amati, M. Ciafaloni and G. Veneziano,Planckian scattering beyond the semiclassical approximation,Phys. Lett. B289(1992) 87

  18. [18]

    Di Vecchia, C

    P. Di Vecchia, C. Heissenberg, R. Russo and G. Veneziano,The gravitational eikonal: From particle, string and brane collisions to black-hole encounters,Phys. Rept.1083(2024) 1 [2306.16488]

  19. [19]

    Aichelburg and R.U

    P.C. Aichelburg and R.U. Sexl,On the Gravitational field of a massless particle,Gen. Rel. Grav.2(1971) 303. – 34 –

  20. [20]

    Giacchini and T.d.P

    B.L. Giacchini and T.d.P. Netto,Effective delta sources and regularity in higher-derivative and ghost-free gravity,Journal of Cosmology and Astroparticle Physics2019(2019) 013–013

  21. [21]

    Boos, V.P

    J. Boos, V.P. Frolov and A. Zelnikov,Gravitational field of static p -branes in linearized ghost-free gravity,Phys. Rev. D97(2018) 084021 [1802.09573]

  22. [22]

    Buoninfante, G

    L. Buoninfante, G. Harmsen, S. Maheshwari and A. Mazumdar,Nonsingular metric for an electrically charged point-source in ghost-free infinite derivative gravity,Phys. Rev. D98 (2018) 084009 [1804.09624]

  23. [23]

    Giacchini and T

    B.L. Giacchini and T. de Paula Netto,Weak-field limit and regular solutions in polynomial higher-derivative gravities,Eur. Phys. J. C79(2019) 217 [1806.05664]

  24. [24]

    Kol´ aˇ r and A

    I. Kol´ aˇ r and A. Mazumdar,NUT charge in linearized infinite derivative gravity,Phys. Rev. D101(2020) 124005 [2004.07613]

  25. [25]

    Modesto, J

    L. Modesto, J.W. Moffat and P. Nicolini,Black holes in an ultraviolet complete quantum gravity,Phys. Lett. B695(2011) 397 [1010.0680]

  26. [26]

    Nonlocal star as a blackhole mimicker,

    L. Buoninfante and A. Mazumdar,Nonlocal star as a blackhole mimicker,Phys. Rev. D 100(2019) 024031 [1903.01542]

  27. [27]

    Bambi, D

    C. Bambi, D. Malafarina and L. Modesto,Terminating black holes in asymptotically free quantum gravity,Eur. Phys. J. C74(2014) 2767 [1306.1668]

  28. [28]

    Koshelev and A

    A.S. Koshelev and A. Tokareva,Nonperturbative quantum gravity denounces singular black holes,Phys. Rev. D111(2025) 086026 [2404.07925]

  29. [29]

    Buoninfante, A

    L. Buoninfante, A.S. Koshelev, G. Lambiase and A. Mazumdar,Classical properties of non-local, ghost- and singularity-free gravity,JCAP09(2018) 034 [1802.00399]

  30. [30]

    Edholm, A.S

    J. Edholm, A.S. Koshelev and A. Mazumdar,Behavior of the Newtonian potential for ghost-free gravity and singularity-free gravity,Phys. Rev. D94(2016) 104033 [1604.01989]

  31. [31]

    Koshelev, J

    A.S. Koshelev, J. Marto and A. Mazumdar,Schwarzschild1/r-singularity is not permissible in ghost free quadratic curvature infinite derivative gravity,Phys. Rev. D98(2018) 064023 [1803.00309]

  32. [32]

    Higher-order regularity in local and nonlocal quantum gravity,

    N. Burzill` a, B.L. Giacchini, T.d.P. Netto and L. Modesto,Higher-order regularity in local and nonlocal quantum gravity,Eur. Phys. J. C81(2021) 462 [2012.11829]

  33. [33]

    Giacchini,On the cancellation of Newtonian singularities in higher-derivative gravity, Phys

    B.L. Giacchini,On the cancellation of Newtonian singularities in higher-derivative gravity, Phys. Lett. B766(2017) 306 [1609.05432]

  34. [34]

    Boos,Effects of Non-locality in Gravity and Quantum Theory, Ph.D

    J. Boos,Effects of Non-locality in Gravity and Quantum Theory, Ph.D. thesis, Alberta U., 2020.2009.10856. 10.7939/r3-7bt0-na76

  35. [35]

    Nonlocality and gravitoelectro- magnetic duality,

    J. Boos and I. Kol´ aˇ r,Nonlocality and gravitoelectromagnetic duality,Phys. Rev. D104 (2021) 024018 [2103.10555]

  36. [36]

    Towards a Non-singular Paradigm of Black Hole Physics

    R. Carballo-Rubio et al.,Towards a non-singular paradigm of black hole physics,JCAP05 (2025) 003 [2501.05505]

  37. [37]

    Cadoni, R

    M. Cadoni, R. Murgia, M. Pitzalis and A.P. Sanna,Quasi-local masses and cosmological coupling of black holes and mimickers,JCAP03(2024) 026 [2309.16444]

  38. [38]

    Cadoni, A

    M. Cadoni, A.P. Sanna, M. Pitzalis, B. Banerjee, R. Murgia, N. Hazra et al.,Cosmological coupling of nonsingular black holes,JCAP11(2023) 007 [2306.11588]. – 35 –

  39. [39]

    Cadoni, M

    M. Cadoni, M. Pitzalis and A.P. Sanna,Apparent horizons in cosmologically-embedded black holes,JCAP02(2025) 051 [2410.10459]

  40. [40]

    Cadoni, L

    M. Cadoni, L. de Lima, M. Pitzalis, D.C. Rodrigues and A.P. Sanna,Cosmologically Coupled Black Holes with Regular Horizons,2601.03296

  41. [41]

    Bardeen,Non-singular general-relativistic gravitational collapse,Proc

    J.M. Bardeen,Non-singular general-relativistic gravitational collapse,Proc. Int. Conf. GR5, 174(1968)

  42. [42]

    Dymnikova,Vacuum nonsingular black hole,Gen

    I. Dymnikova,Vacuum nonsingular black hole,Gen. Rel. Grav.24(1992) 235

  43. [43]

    Formation and evaporation of non-singular black holes

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

  44. [44]

    The Bardeen Model as a Nonlinear Magnetic Monopole

    E. Ayon-Beato and A. Garcia,The Bardeen model as a nonlinear magnetic monopole,Phys. Lett. B493(2000) 149 [gr-qc/0009077]

  45. [45]

    Regular Magnetic Black Holes and Monopoles from Nonlinear Electrodynamics

    K.A. Bronnikov,Regular magnetic black holes and monopoles from nonlinear electrodynamics,Phys. Rev. D63(2001) 044005 [gr-qc/0006014]

  46. [46]

    Carballo-Rubio, F

    R. Carballo-Rubio, F. Di Filippo, S. Liberati, C. Pacilio and M. Visser,On the viability of regular black holes,JHEP07(2018) 023 [1805.02675]

  47. [47]

    Carballo-Rubio, F

    R. Carballo-Rubio, F. Di Filippo, S. Liberati, C. Pacilio and M. Visser,Regular black holes without mass inflation instability,JHEP09(2022) 118 [2205.13556]

  48. [48]

    C. Lan, H. Yang, Y. Guo and Y.-G. Miao,Regular Black Holes: A Short Topic Review,Int. J. Theor. Phys.62(2023) 202 [2303.11696]

  49. [49]

    Bambi, ed.,Regular Black Holes

    C. Bambi, ed.,Regular Black Holes. Towards a New Paradigm of Gravitational Collapse, Springer Series in Astrophysics and Cosmology, Springer (2023), 10.1007/978-981-99-1596-5, [2307.13249]

  50. [50]

    Lee-Wick black holes,

    C. Bambi, L. Modesto and Y. Wang,Lee–Wick black holes,Phys. Lett. B764(2017) 306 [1611.03650]

  51. [51]

    Newtonian potential in higher-derivative quantum gravity,

    N. Burzill` a, B.L. Giacchini, T.d.P. Netto and L. Modesto,Newtonian potential in higher-derivative quantum gravity,Phys. Rev. D103(2021) 064080 [2012.06254]

  52. [52]

    Action principle selection of regular black holes,

    B.L. Giacchini, T.d.P. Netto and L. Modesto,Action principle selection of regular black holes,Phys. Rev. D104(2021) 084072 [2105.00300]

  53. [53]

    Z. Mo, T. de Paula Netto, N. Burzill` a and L. Modesto,Stringballs and Planckballs for dark matter,JHEP07(2022) 131 [2202.04540]

  54. [54]

    Geodesic incompleteness of some popular regular black holes,

    T. Zhou and L. Modesto,Geodesic incompleteness of some popular regular black holes, Phys. Rev. D107(2023) 044016 [2208.02557]

  55. [55]

    On the analytic extension of regular rotating black holes,

    T. Zhou and L. Modesto,On the analytic extension of regular rotating black holes, 2303.11322

  56. [56]

    On effective models of regular black holes inspired by higher-derivative and nonlocal gravity,

    T. de Paula Netto, B.L. Giacchini, N. Burzill` a and L. Modesto,On effective models of regular black holes inspired by higher-derivative and nonlocal gravity,Nucl. Phys. B1007 (2024) 116674 [2308.12251]

  57. [57]

    Regular multi-horizon Lee-Wick black holes,

    N. Burzill` a, B.L. Giacchini, T. de Paula Netto and L. Modesto,Regular multi-horizon Lee-Wick black holes,JCAP11(2023) 067 [2308.12810]

  58. [58]

    Universal leading quantum correction to the Newton potential,

    T. de Paula Netto, L. Modesto and I.L. Shapiro,Universal leading quantum correction to the Newton potential,Eur. Phys. J. C82(2022) 160 [2110.14263]. – 36 –

  59. [59]

    Bueno, P.A

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

  60. [60]

    Bueno, P

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

  61. [61]

    Fernandes,Regular BTZ black holes from an infinite tower of corrections,Phys

    P.G.S. Fernandes,Regular BTZ black holes from an infinite tower of corrections,Phys. Lett. B868(2025) 139772 [2504.08565]

  62. [62]

    Fernandes, J

    P.G.S. Fernandes, J. Gou, L. Heisenberg and N. Nussbaumer,Inflation, black holes with primary hair, and regular planar black holes from an infinite tower of regularized Lovelock-Proca corrections,2511.22798

  63. [63]

    Eichhorn and P

    A. Eichhorn and P.G.S. Fernandes,Regular black holes without mass-inflation instability and gravastars from modified gravity,Phys. Rev. D113(2026) L081501 [2508.00686]

  64. [64]

    Bueno, R.A

    P. Bueno, R.A. Hennigar, ´A.J. Murcia and A. Vicente-Cano,Regular Geometries from Singular Matter in Quasi-Topological Gravity,2603.10110

  65. [65]

    Cadoni and A

    M. Cadoni and A.P. Sanna,Nonsingular black holes from conformal symmetries,Class. Quant. Grav.40(2023) 145012 [2302.06401]

  66. [66]

    Cadoni, M

    M. Cadoni, M. Oi and A.P. Sanna,Evaporation and information puzzle for 2D nonsingular asymptotically flat black holes,JHEP06(2023) 211 [2303.05557]

  67. [67]

    Cadoni, M

    M. Cadoni, M. Oi and A.P. Sanna,Effective models of nonsingular quantum black holes, Phys. Rev. D106(2022) 024030 [2204.09444]

  68. [68]

    A. Akil, M. Cadoni, L. Modesto, M. Oi and A.P. Sanna,Semiclassical spacetimes at super-Planckian scales from delocalized sources,Phys. Rev. D108(2023) 044051 [2211.01657]

  69. [69]

    Bonanno, M

    A. Bonanno, M. Cadoni, M. Pitzalis and A.P. Sanna,Effective quantum spacetimes from functional renormalization group,Phys. Rev. D111(2025) 064031 [2410.16866]

  70. [70]

    Wataghin,Bemerkung ¨ uber die Selbstenergie der Elektronen,Z

    G. Wataghin,Bemerkung ¨ uber die Selbstenergie der Elektronen,Z. Phys.88(1934) 92

  71. [71]

    Kostelecky and S

    V.A. Kostelecky and S. Samuel,On a Nonperturbative Vacuum for the Open Bosonic String,Nucl. Phys. B336(1990) 263

  72. [72]

    Ohmori,A Review on tachyon condensation in open string field theories, master thesis, Department of Physics, Faculty of Science, University of Tokyo, 2, 2001, [hep-th/0102085]

    K. Ohmori,A Review on tachyon condensation in open string field theories, master thesis, Department of Physics, Faculty of Science, University of Tokyo, 2, 2001, [hep-th/0102085]

  73. [73]

    Barvinsky,Dark energy and dark matter from non- local ghost-free gravity theory,Phys

    A.O. Barvinsky,Dark energy and dark matter from nonlocal ghost-free gravity theory,Phys. Lett. B710(2012) 12 [1107.1463]

  74. [74]

    Deser and R

    S. Deser and R.P. Woodard,Nonlocal Cosmology,Phys. Rev. Lett.99(2007) 111301 [0706.2151]

  75. [75]

    Non-local gravity and dark energy

    M. Maggiore and M. Mancarella,Nonlocal gravity and dark energy,Phys. Rev. D90(2014) 023005 [1402.0448]

  76. [76]

    Anselmi,Renormalization and causality violations in classical gravity coupled with quantum matter,JHEP01(2007) 062 [hep-th/0605205]

    D. Anselmi,Renormalization and causality violations in classical gravity coupled with quantum matter,JHEP01(2007) 062 [hep-th/0605205]

  77. [77]

    Don` a, S

    P. Don` a, S. Giaccari, L. Modesto, L. Rachwal and Y. Zhu,Scattering amplitudes in super-renormalizable gravity,JHEP08(2015) 038 [1506.04589]

  78. [78]

    Modesto and G

    L. Modesto and G. Calcagni,Tree-level scattering amplitudes in nonlocal field theories, JHEP10(2021) 169 [2107.04558]. – 37 –

  79. [79]

    Causality in Nonlocal Gravity,

    S. Giaccari and L. Modesto,Causality in Nonlocal Gravity, in10th MATHEMATICAL PHYSICS MEETING: School and Conference on Modern Mathematical Physics, pp. 121–136, 2020 [1803.08748]

  80. [80]

    Buoninfante and B.L

    L. Buoninfante and B.L. Giacchini,Light bending by a slowly rotating source in quadratic theories of gravity,Phys. Rev. D102(2020) 024020 [2005.05355]

Showing first 80 references.