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arxiv: 2502.13208 · v2 · pith:QMT7DLKDnew · submitted 2025-02-18 · ✦ hep-th · gr-qc· math-ph· math.MP· quant-ph

Finite cutoff JT gravity: Baby universes, Matrix dual, and (Krylov) Complexity

Pith reviewed 2026-05-23 02:23 UTC · model grok-4.3

classification ✦ hep-th gr-qcmath-phmath.MPquant-ph
keywords finite cutoff JT gravityEinstein-Rosen bridgebaby universesmatrix model dualKrylov complexitycomplexity-volume proposalspectral deformationmoduli space volume
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The pith

Finite cutoff deforms JT gravity so the Einstein-Rosen bridge saturates faster than in the pure theory.

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

The paper applies the complexity=volume conjecture to JT gravity with a finite radial cutoff, which introduces an integrable irrelevant deformation. This deformation changes the spectrum of the dual matrix model and causes the late-time growth of the black-hole interior to saturate sooner than in the undeformed case. The same deformation modifies the emission rate of baby universes once Lorentzian time evolution is turned on, and the relative saturation time depends on the inverse temperature. The work also examines how the cutoff alters the dual matrix model, including possible one-cut universality and non-perturbative shifts in the volume of the moduli space.

Core claim

In finite-cutoff JT gravity the length of the Einstein-Rosen bridge saturates at late times more rapidly than in pure JT gravity because the integrable irrelevant deformation modifies the spectral properties non-trivially; the saturation time relative to the undeformed theory depends on the inverse temperature, the probability of baby-universe emission changes only when Lorentzian evolution is activated, and the dual matrix model exhibits one-cut universality together with non-perturbative corrections to the moduli-space volume induced by the deformed spectral curve.

What carries the argument

The integrable irrelevant deformation generated by the finite radial cutoff, which alters the spectral curve of the matrix-model dual and thereby controls late-time volume growth.

If this is right

  • The deformation parameter controls how quickly the interior volume stops growing.
  • Baby-universe emission rates receive a deformation correction only under Lorentzian evolution.
  • The relative saturation time between deformed and undeformed theories varies with temperature.
  • Non-perturbative corrections appear in the volume of the moduli space through changes to the spectral curve.

Where Pith is reading between the lines

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

  • The temperature dependence of saturation time may produce distinct late-time signatures in thermal ensembles of the deformed theory.
  • If Krylov complexity tracks ERB length in the deformed model, the same faster saturation should appear in operator growth measures.
  • The one-cut universality noted in the matrix dual could simplify calculations of other observables once the cutoff is fixed.

Load-bearing premise

The complexity-equals-volume proposal continues to hold without modification inside the finite-cutoff deformed theory.

What would settle it

An explicit calculation of the late-time ERB length in the finite-cutoff model that shows the same saturation time as pure JT gravity would falsify the central claim.

read the original abstract

In this paper, as an application of the `Complexity = Volume' proposal, we calculate the growth of the interior of a black hole at late times for finite cutoff JT gravity. Due to this integrable, irrelevant deformation, the spectral properties are modified non-trivially. The Einstein-Rosen Bridge (ERB) length saturates faster than pure JT gravity. We comment on the possible connection between Krylov Complexity and ERB length for the deformed theory. Apart from this, we compute the emission probability of baby universes in the deformed theory and find that it changes due to the deformation parameter only if we turn on Lorentzian evolution. We also find that the saturation time of the deformed theory relative to the undeformed one depends on the inverse temperature. We also highlight the subtleties involved in the dual matrix model and comment on the possible one-cut universality. Finally, we comment on the possible correction to the volume of the moduli space arising from the non-perturbative correction of the spectral curve induced by the finite boundary cutoff.

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

1 major / 2 minor

Summary. The manuscript applies the Complexity=Volume proposal to finite-cutoff JT gravity deformed by an integrable irrelevant operator. It claims that the ERB length saturates faster than in pure JT gravity due to modified spectral properties, computes baby-universe emission probabilities that depend on the deformation parameter only under Lorentzian evolution, discusses subtleties in the dual matrix model and possible one-cut universality, comments on a possible link between Krylov complexity and ERB length, and notes potential non-perturbative corrections to the moduli-space volume arising from the deformed spectral curve.

Significance. If the central assumption holds, the work supplies a concrete illustration of how an irrelevant deformation alters late-time interior growth and complexity measures in a solvable 2d gravity model. The reported inverse-temperature dependence of the relative saturation time and the matrix-model analysis could inform studies of deformed JT gravity and its holographic duals.

major comments (1)
  1. [ERB length calculation and Complexity=Volume application] The headline claim that the ERB length saturates faster is obtained by applying the standard, unmodified Complexity=Volume dictionary directly to the deformed geometry and spectral curve. The manuscript does not derive a corrected dictionary or demonstrate that the volume operator remains invariant under the irrelevant deformation, which is load-bearing for linking the deformation parameter to the observed saturation time.
minor comments (2)
  1. [Abstract] The abstract states that saturation time depends on inverse temperature but does not give the functional form; including the explicit dependence in the main text would improve clarity.
  2. [Baby universe emission section] The discussion of baby-universe emission probabilities would benefit from an explicit formula showing how the deformation parameter enters only in the Lorentzian case.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading and constructive feedback. We respond to the single major comment below.

read point-by-point responses
  1. Referee: The headline claim that the ERB length saturates faster is obtained by applying the standard, unmodified Complexity=Volume dictionary directly to the deformed geometry and spectral curve. The manuscript does not derive a corrected dictionary or demonstrate that the volume operator remains invariant under the irrelevant deformation, which is load-bearing for linking the deformation parameter to the observed saturation time.

    Authors: We agree that the manuscript applies the standard Complexity=Volume proposal without deriving a modified dictionary from the deformed boundary theory. The ERB length is obtained by evaluating the volume of the maximal slice using the geometry whose properties are determined by the deformed spectral curve; the deformation enters through this modified geometry rather than through an altered dictionary. Because the volume is a purely geometric quantity, we take the standard dictionary to remain applicable at leading order for this integrable deformation. We have added a short clarifying paragraph in the introduction (new paragraph after Eq. (2.3)) stating the assumption explicitly and noting that a first-principles derivation of the dictionary under the irrelevant operator lies outside the present scope. revision: partial

Circularity Check

0 steps flagged

No significant circularity; C=V applied as external proposal

full rationale

The derivation applies the Complexity=Volume proposal (an external assumption) to compute ERB length in the finite-cutoff deformed JT gravity, where the deformation modifies the spectral curve and late-time properties. Saturation times and baby-universe emission probabilities are computed from the deformed geometry under this dictionary; no equation defines the output in terms of itself, no fitted parameter is relabeled as a prediction, and no self-citation chain is invoked to justify the central dictionary. The result is a direct calculation under stated assumptions rather than a reduction to inputs by construction.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

Abstract-only review yields an incomplete ledger; the central claims rest on the complexity=volume proposal and standard JT-gravity assumptions whose details are not visible.

free parameters (1)
  • deformation parameter
    Finite cutoff introduces a parameter that modifies spectral properties and saturation times.
axioms (1)
  • domain assumption Complexity equals volume proposal
    Invoked to equate interior growth with ERB length.

pith-pipeline@v0.9.0 · 5734 in / 1102 out tokens · 55335 ms · 2026-05-23T02:23:13.848879+00:00 · methodology

discussion (0)

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Forward citations

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Reference graph

Works this paper leans on

119 extracted references · 119 canonical work pages · cited by 2 Pith papers · 46 internal anchors

  1. [1]

    J. M. Maldacena, The Large N limit of superconformal field theories and supergravity , Adv. Theor. Math. Phys. 2 (1998) 231–252 [ hep-th/9711200]

  2. [2]

    Anti De Sitter Space And Holography

    E. Witten, Anti-de Sitter space and holography , Adv. Theor. Math. Phys. 2 (1998) 253–291 [hep-th/9802150]

  3. [3]

    Jackiw, Lower Dimensional Gravity, Nucl

    R. Jackiw, Lower Dimensional Gravity, Nucl. Phys. B 252 (1985) 343–356

  4. [4]

    Teitelboim, Gravitation and Hamiltonian Structure in Two Space-Time Dimensions , Phys

    C. Teitelboim, Gravitation and Hamiltonian Structure in Two Space-Time Dimensions , Phys. Lett. B 126 (1983) 41–45

  5. [5]

    Models of AdS_2 Backreaction and Holography

    A. Almheiri and J. Polchinski, Models of AdS 2 backreaction and holography, JHEP 11 (2015) 014 [1402.6334]

  6. [6]

    Quantum Gravity Partition Functions in Three Dimensions

    A. Maloney and E. Witten, Quantum Gravity Partition Functions in Three Dimensions , JHEP 02 (2010) 029 [ 0712.0155]

  7. [7]

    Partition Functions of Three-Dimensional Pure Gravity

    X. Yin, Partition Functions of Three-Dimensional Pure Gravity , Commun. Num. Theor. Phys. 2 (2008) 285–324 [ 0710.2129]

  8. [8]

    Collier, L

    S. Collier, L. Eberhardt and M. Zhang, Solving 3d gravity with Virasoro TQFT , SciPost Phys. 15 (2023), no. 4, 151 [ 2304.13650]

  9. [9]

    de Boer, D

    J. de Boer, D. Liska and B. Post, Multiboundary wormholes and OPE statistics , JHEP 10 (2024) 207 [ 2405.13111]

  10. [10]

    Collier, L

    S. Collier, L. Eberhardt and M. Zhang, 3d gravity from Virasoro TQFT: Holography, wormholes and knots , SciPost Phys. 17 (2024), no. 5, 134 [ 2401.13900]

  11. [11]

    Bhattacharyya, S

    A. Bhattacharyya, S. Ghosh, P. Nandi and S. Pal, 3D N = 1 supergravity from Virasoro TQFT: gravitational partition function and Out-of-time-order correlator , JHEP 02 (2025) 027 [2408.01538]. – 36 –

  12. [12]

    Post and I

    B. Post and I. Tsiares, A non-rational Verlinde formula from Virasoro TQFT , 2411.07285

  13. [13]

    Takahashi, Anyon Condensation in Virasoro TQFT: Wormhole Factorization , 2412.11486

    S. Takahashi, Anyon Condensation in Virasoro TQFT: Wormhole Factorization , 2412.11486

  14. [14]

    T. G. Mertens and G. J. Turiaci, Solvable models of quantum black holes: a review on Jackiw–Teitelboim gravity, Living Rev. Rel. 26 (2023), no. 1, 4 [ 2210.10846]

  15. [15]

    Moitra, S

    U. Moitra, S. K. Sake, S. P. Trivedi and V. Vishal, Jackiw-Teitelboim Gravity and Rotating Black Holes, JHEP 11 (2019) 047 [ 1905.10378]

  16. [16]

    Moitra, S

    U. Moitra, S. K. Sake and S. P. Trivedi, Aspects of Jackiw-Teitelboim gravity in Anti-de Sitter and de Sitter spacetime , JHEP 06 (2022) 138 [ 2202.03130]

  17. [17]

    Gapless Spin-Fluid Ground State in a Random Quantum Heisenberg Magnet

    S. Sachdev and J. Ye, Gapless spin fluid ground state in a random, quantum Heisenberg magnet, Phys. Rev. Lett. 70 (1993) 3339 [ cond-mat/9212030]

  18. [18]

    Kitaev, A simple model of quantum holography (part 1)

    A. Kitaev, A simple model of quantum holography (part 1). Kavli Institute for Theoretical Physics Program: Entanglement in Strongly-Correlated Quantum Matter (Apr 6 - Jul 2, 2015). Online at https://online.kitp.ucsb.edu/online/entangled15/kitaev/, Apr., 2015

  19. [19]

    Kitaev, A simple model of quantum holography (part 2)

    A. Kitaev, A simple model of quantum holography (part 2). Kavli Institute for Theoretical Physics Program: Entanglement in Strongly-Correlated Quantum Matter (Apr 6 - Jul 2, 2015). Online at https://online.kitp.ucsb.edu/online/entangled15/kitaev2/, May, 2015

  20. [20]

    Bekenstein-Hawking Entropy and Strange Metals

    S. Sachdev, Bekenstein-Hawking Entropy and Strange Metals , Phys. Rev. X 5 (2015), no. 4, 041025 [1506.05111]

  21. [21]

    S. H. Shenker and D. Stanford, Stringy effects in scrambling, JHEP 05 (2015) 132 [1412.6087]

  22. [22]

    A bound on chaos

    J. Maldacena, S. H. Shenker and D. Stanford, A bound on chaos , JHEP 08 (2016) 106 [1503.01409]

  23. [23]

    Stanford, Many-body chaos at weak coupling , JHEP 10 (2016) 009 [ 1512.07687]

    D. Stanford, Many-body chaos at weak coupling , JHEP 10 (2016) 009 [ 1512.07687]

  24. [24]

    J. S. Cotler, G. Gur-Ari, M. Hanada, J. Polchinski, P. Saad, S. H. Shenker, D. Stanford, A. Streicher and M. Tezuka, Black Holes and Random Matrices , JHEP 05 (2017) 118 [1611.04650], [Erratum: JHEP 09, 002 (2018)]

  25. [25]

    Chaos in AdS$_2$ holography

    K. Jensen, Chaos in AdS 2 Holography, Phys. Rev. Lett. 117 (2016), no. 11, 111601 [1605.06098]

  26. [26]

    An Investigation of AdS$_2$ Backreaction and Holography

    J. Engels¨ oy, T. G. Mertens and H. Verlinde,An investigation of AdS 2 backreaction and holography, JHEP 07 (2016) 139 [ 1606.03438]

  27. [27]

    Onset of many-body chaos in the $O(N)$ model

    D. Chowdhury and B. Swingle, Onset of many-body chaos in the O(N) model, Phys. Rev. D 96 (2017), no. 6, 065005 [ 1703.02545]

  28. [28]

    Altland, B

    A. Altland, B. Post, J. Sonner, J. van der Heijden and E. P. Verlinde, Quantum chaos in 2D gravity, SciPost Phys. 15 (2023), no. 2, 064 [ 2204.07583]

  29. [29]

    Comments on the Sachdev-Ye-Kitaev model

    J. Maldacena and D. Stanford, Remarks on the Sachdev-Ye-Kitaev model , Phys. Rev. D 94 (2016), no. 10, 106002 [ 1604.07818]

  30. [30]

    Conformal symmetry and its breaking in two dimensional Nearly Anti-de-Sitter space

    J. Maldacena, D. Stanford and Z. Yang, Conformal symmetry and its breaking in two dimensional Nearly Anti-de-Sitter space , PTEP 2016 (2016), no. 12, 12C104 [ 1606.01857]

  31. [31]

    Pure states in the SYK model and nearly-$AdS_2$ gravity

    I. Kourkoulou and J. Maldacena, Pure states in the SYK model and nearly- AdS2 gravity, 1707.02325. – 37 –

  32. [32]

    The soft mode in the Sachdev-Ye-Kitaev model and its gravity dual

    A. Kitaev and S. J. Suh, The soft mode in the Sachdev-Ye-Kitaev model and its gravity dual , JHEP 05 (2018) 183 [ 1711.08467]

  33. [33]

    T. G. Mertens, The Schwarzian theory — origins , JHEP 05 (2018) 036 [ 1801.09605]

  34. [34]

    H. W. Lin, J. Maldacena and Y. Zhao, Symmetries Near the Horizon , JHEP 08 (2019) 049 [1904.12820]

  35. [35]

    P. Saad, S. H. Shenker and D. Stanford, A semiclassical ramp in SYK and in gravity , 1806.06840

  36. [36]

    P. Saad, S. H. Shenker and D. Stanford, JT gravity as a matrix integral , 1903.11115

  37. [37]

    Stanford and E

    D. Stanford and E. Witten, JT gravity and the ensembles of random matrix theory , Adv. Theor. Math. Phys. 24 (2020), no. 6, 1475–1680 [ 1907.03363]

  38. [38]

    Weil-Petersson volume of moduli spaces, Mirzakhani's recursion and matrix models

    B. Eynard and N. Orantin, Weil-Petersson volume of moduli spaces, Mirzakhani’s recursion and matrix models , 0705.3600

  39. [39]

    S. W. Hawking, Breakdown of Predictability in Gravitational Collapse , Phys. Rev. D 14 (1976) 2460–2473

  40. [40]

    S. D. Mathur, The Information paradox: A Pedagogical introduction , Class. Quant. Grav. 26 (2009) 224001 [ 0909.1038]

  41. [41]

    Raju, Lessons from the information paradox , Phys

    S. Raju, Lessons from the information paradox , Phys. Rept. 943 (2022) 1–80 [ 2012.05770]

  42. [42]

    J. M. Maldacena, Eternal black holes in anti-de Sitter , JHEP 04 (2003) 021 [hep-th/0106112]

  43. [43]

    The Trouble with de Sitter Space

    N. Goheer, M. Kleban and L. Susskind, The Trouble with de Sitter space , JHEP 07 (2003) 056 [hep-th/0212209]

  44. [44]

    Disturbing Implications of a Cosmological Constant

    L. Dyson, M. Kleban and L. Susskind, Disturbing implications of a cosmological constant , JHEP 10 (2002) 011 [ hep-th/0208013]

  45. [45]

    J. L. F. Barbon and E. Rabinovici, Very long time scales and black hole thermal equilibrium , JHEP 11 (2003) 047 [ hep-th/0308063]

  46. [46]

    Prange, The spectral form factor is not self-averaging , Physical review letters 78 (1997), no

    R. Prange, The spectral form factor is not self-averaging , Physical review letters 78 (1997), no. 12, 2280

  47. [47]

    Yang, The Quantum Gravity Dynamics of Near Extremal Black Holes , JHEP 05 (2019) 205, [ 1809.08647]

    Z. Yang, The Quantum Gravity Dynamics of Near Extremal Black Holes , JHEP 05 (2019) 205 [1809.08647]

  48. [48]

    D. J. Gross and V. Rosenhaus, All point correlation functions in SYK , JHEP 12 (2017) 148 [1710.08113]

  49. [49]

    H. T. Lam, T. G. Mertens, G. J. Turiaci and H. Verlinde, Shockwave S-matrix from Schwarzian Quantum Mechanics , JHEP 11 (2018) 182 [ 1804.09834]

  50. [50]

    T. G. Mertens, G. J. Turiaci and H. L. Verlinde, Solving the Schwarzian via the Conformal Bootstrap, JHEP 08 (2017) 136 [ 1705.08408]

  51. [51]

    The Schwarzian Theory - A Wilson Line Perspective

    A. Blommaert, T. G. Mertens and H. Verschelde, The Schwarzian Theory - A Wilson Line Perspective, JHEP 12 (2018) 022 [ 1806.07765]

  52. [52]

    Blommaert, T

    A. Blommaert, T. G. Mertens and H. Verschelde, Clocks and Rods in Jackiw-Teitelboim Quantum Gravity, JHEP 09 (2019) 060 [ 1902.11194]. – 38 –

  53. [53]

    Bulycheva, Semiclassical correlators in Jackiw-Teitelboim gravity, JHEP 11 (2019) 023 [1905.05692]

    K. Bulycheva, Semiclassical correlators in Jackiw-Teitelboim gravity, JHEP 11 (2019) 023 [1905.05692]

  54. [54]

    L. V. Iliesiu, S. S. Pufu, H. Verlinde and Y. Wang, An exact quantization of Jackiw-Teitelboim gravity, JHEP 11 (2019) 091 [ 1905.02726]

  55. [55]

    G. V. Lavrelashvili, V. A. Rubakov and P. G. Tinyakov, Disruption of Quantum Coherence upon a Change in Spatial Topology in Quantum Gravity , JETP Lett. 46 (1987) 167–169

  56. [56]

    Hawking, Quantum coherence down the wormhole , Physics Letters B 195 (1987), no

    S. Hawking, Quantum coherence down the wormhole , Physics Letters B 195 (1987), no. 3, 337–343

  57. [57]

    S. B. Giddings and A. Strominger, Axion-induced topology change in quantum gravity and string theory, Nuclear Physics B 306 (1988), no. 4, 890–907

  58. [58]

    S. R. Coleman, Black Holes as Red Herrings: Topological Fluctuations and the Loss of Quantum Coherence, Nucl. Phys. B 307 (1988) 867–882

  59. [59]

    Coleman, Why there is nothing rather than something: A theory of the cosmological constant, Nuclear Physics B 310 (1988), no

    S. Coleman, Why there is nothing rather than something: A theory of the cosmological constant, Nuclear Physics B 310 (1988), no. 3, 643–668

  60. [60]

    S. B. Giddings and A. Strominger, Baby universe, third quantization and the cosmological constant, Nuclear Physics B 321 (1989), no. 2, 481–508

  61. [61]

    Klebanov, L

    I. Klebanov, L. Susskind and T. Banks, Wormholes and the cosmological constant , Nuclear Physics B 317 (1989), no. 3, 665–692

  62. [62]

    J. M. Maldacena and L. Maoz, Wormholes in AdS , JHEP 02 (2004) 053 [ hep-th/0401024]

  63. [63]

    Euclidean Wormholes in String Theory

    N. Arkani-Hamed, J. Orgera and J. Polchinski, Euclidean wormholes in string theory , JHEP 12 (2007) 018 [ 0705.2768]

  64. [64]

    Chaos and Quantum Thermalization

    M. Srednicki, Chaos and Quantum Thermalization , Phys. Rev. E 50 (3, 1994) [cond-mat/9403051]

  65. [65]

    J. M. Deutsch, Quantum statistical mechanics in a closed system , Phys. Rev. A 43 (1991), no. 4, 2046

  66. [66]

    Saad, Late Time Correlation Functions, Baby Universes, and ETH in JT Gravity , 1910.10311

    P. Saad, Late Time Correlation Functions, Baby Universes, and ETH in JT Gravity , 1910.10311

  67. [67]

    A. B. Zamolodchikov, Expectation value of composite field T anti-T in two-dimensional quantum field theory, hep-th/0401146

  68. [68]

    F. A. Smirnov and A. B. Zamolodchikov, On space of integrable quantum field theories , Nucl. Phys. B 915 (2017) 363–383 [ 1608.05499]

  69. [69]

    $T \bar{T}$-deformed 2D Quantum Field Theories

    A. Cavagli` a, S. Negro, I. M. Sz´ ecs´ enyi and R. Tateo,T ¯T -deformed 2D Quantum Field Theories, JHEP 10 (2016) 112 [ 1608.05534]

  70. [70]

    Generalised Born-Infeld models, Lax operators and the $\textrm{T} \bar{\textrm{T}}$ perturbation

    R. Conti, L. Iannella, S. Negro and R. Tateo, Generalised Born-Infeld models, Lax operators and the TT perturbation, JHEP 11 (2018) 007 [ 1806.11515]

  71. [71]

    The $\textrm{T}\bar{\textrm{T}}$ perturbation and its geometric interpretation

    R. Conti, S. Negro and R. Tateo, The TT perturbation and its geometric interpretation , JHEP 02 (2019) 085 [ 1809.09593]

  72. [72]

    Conti, S

    R. Conti, S. Negro and R. Tateo, Conserved currents and T ¯Ts irrelevant deformations of 2D integrable field theories, JHEP 11 (2019) 120 [ 1904.09141]. – 39 –

  73. [73]

    Guica, R

    M. Guica, R. Monten and I. Tsiares, Classical and quantum symmetries of T ¯T -deformed CFTs, 2212.14014

  74. [74]

    Morone, S

    T. Morone, S. Negro and R. Tateo, Gravity and T ¯T flows in higher dimensions , Nucl. Phys. B 1005 (2024) 116605 [ 2401.16400]

  75. [75]

    Bielli, C

    D. Bielli, C. Ferko, L. Smith and G. Tartaglino-Mazzucchelli, T-Duality and T T -like Deformations of Sigma Models , 2407.11636

  76. [76]

    Chang, S

    J.-C. Chang, S. He, Y.-X. Liu and L. Zhao, The holographic T ¯T deformation of the entanglement entropy in (A)dS 3/CFT2, 2409.08198

  77. [77]

    Tsolakidis, Massive gravity generalization of T T deformations, JHEP 09 (2024) 167 [2405.07967]

    E. Tsolakidis, Massive gravity generalization of T T deformations, JHEP 09 (2024) 167 [2405.07967]

  78. [78]

    He, One-loop partition functions in T T -deformed AdS3, JHEP 05 (2024) 067 [2401.09879]

    M. He, One-loop partition functions in T T -deformed AdS3, JHEP 05 (2024) 067 [2401.09879]

  79. [79]

    Babaei-Aghbolagh, S

    H. Babaei-Aghbolagh, S. He and H. Ouyang, Generalized T ¯T -like flows for scalar theories in two dimensions, 2501.14583

  80. [80]

    Jiang, A pedagogical review on solvable irrelevant deformations of 2D quantum field theory , Commun

    Y. Jiang, A pedagogical review on solvable irrelevant deformations of 2D quantum field theory , Commun. Theor. Phys. 73 (2021), no. 5, 057201 [ 1904.13376]

Showing first 80 references.