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arxiv: 2604.03003 · v1 · submitted 2026-04-03 · ✦ hep-th · gr-qc

Black Hole Interior Operators and Dilatation Symmetry in Planar Black Branes

Pith reviewed 2026-05-13 18:06 UTC · model grok-4.3

classification ✦ hep-th gr-qc
keywords black hole interiorAdS black branesmirror operatorsdilatation symmetryscaling covariancebulk reconstructionstate-dependent operators
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The pith

Mirror operators for black hole interiors satisfy the dilatation covariance condition required by planar AdS black branes.

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

Planar AdS black branes possess a scaling symmetry that maps solutions at one temperature to solutions at another. Boundary representations of bulk interior modes are therefore expected to inherit this symmetry, meaning their correlators must transform covariantly under boundary dilatations. The paper derives the precise covariance condition that any such representation must obey. It then verifies that the state-dependent mirror operators introduced by Papadodimas and Raju satisfy the condition exactly. This establishes that the reconstruction of the black hole interior remains compatible with the brane's scaling symmetry.

Core claim

The Papadodimas-Raju mirror operators satisfy the covariance condition that any boundary representation of interior modes in a planar AdS black brane should satisfy, thereby inheriting the scaling symmetry of the planar black brane despite their state dependence.

What carries the argument

The covariance condition under boundary dilatations, which requires that correlators of interior-mode operators transform according to the scaling symmetry that maps the black brane at one temperature to another.

Load-bearing premise

Boundary representations of bulk interior modes must inherit the scaling symmetry of the planar black brane so that their correlators transform covariantly under dilatations.

What would settle it

An explicit computation of two-point functions of the mirror operators that fails to show the required covariance under a boundary dilatation transformation would falsify the central claim.

read the original abstract

Planar AdS black branes have a scaling symmetry that maps a brane solution at one temperature to a solution at another. It is natural to expect that boundary representations of bulk field modes should inherit this symmetry i.e. their correlators should transform covariantly under boundary dilatations. We derive a covariance condition that any boundary representation of interior modes in a planar AdS black brane should satisfy. We then show that Papadodimas-Raju mirror operators satisfy this condition. Thus the Papadodimas-Raju reconstruction of the bulk interior, although state-dependent, inherits the scaling symmetry of planar AdS black holes.

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 / 1 minor

Summary. The manuscript derives a covariance condition that any boundary representation of interior bulk modes in planar AdS black branes must satisfy, based on the scaling symmetry that maps black-brane solutions at one temperature to solutions at another temperature. It then performs an explicit check showing that the Papadodimas-Raju mirror operators obey this condition, thereby establishing that their state-dependent reconstruction inherits the dilatation symmetry of the planar black branes.

Significance. If the verification holds, the result supplies a non-trivial consistency check for state-dependent bulk reconstructions in the planar limit. It demonstrates that the mirror-operator construction respects a symmetry of the boundary theory without introducing additional parameters, which is relevant for ongoing discussions of black-hole interiors and the information paradox.

major comments (1)
  1. [Main text after covariance condition] The verification that the Papadodimas-Raju operators satisfy the covariance condition (main text, after Eq. (condition)): the substitution into the correlators must be shown in full detail so that it is clear the transformation reduces exactly to the required dilatation factor without relying on additional state-dependent adjustments not already present in the operator definition.
minor comments (1)
  1. [Section deriving covariance condition] Notation for the boundary dilatation generator and the explicit form of the two-point functions used in the check should be defined once at the beginning of the relevant section to improve readability.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the positive assessment and the constructive suggestion for improving the clarity of the verification. We address the comment below and will revise the manuscript accordingly.

read point-by-point responses
  1. Referee: [Main text after covariance condition] The verification that the Papadodimas-Raju operators satisfy the covariance condition (main text, after Eq. (condition)): the substitution into the correlators must be shown in full detail so that it is clear the transformation reduces exactly to the required dilatation factor without relying on additional state-dependent adjustments not already present in the operator definition.

    Authors: We agree that the verification step would benefit from expanded detail. In the revised manuscript we will add an explicit, step-by-step substitution of the Papadodimas-Raju mirror operators into the relevant boundary correlators immediately following Eq. (condition). The calculation will demonstrate that the dilatation transformation produces precisely the required scaling factor, relying solely on the state-dependent definition of the mirror operators and the known transformation properties of the boundary fields, without introducing any further state-dependent adjustments. revision: yes

Circularity Check

0 steps flagged

No significant circularity; derivation is self-contained

full rationale

The paper first derives a covariance condition for boundary representations of interior modes by requiring that their correlators transform appropriately under dilatations induced by the planar black brane scaling symmetry (which maps solutions at different temperatures). It then performs an explicit verification that the independently constructed Papadodimas-Raju mirror operators satisfy this condition. This check does not reduce by the paper's own equations to a quantity already built into the operator definition or to a self-citation chain; the condition is motivated externally by bulk symmetry and the operators are taken from prior work without overlap in authorship. No load-bearing step collapses to a fit, renaming, or ansatz smuggled via self-reference.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The claim rests on the standard holographic dictionary relating bulk fields to boundary operators and on the known scaling symmetry of planar AdS black brane solutions; no new free parameters or invented entities are introduced in the abstract.

axioms (2)
  • domain assumption Planar AdS black branes possess a scaling symmetry that maps a solution at one temperature to a solution at another temperature.
    Invoked in the first sentence of the abstract as the starting point for the covariance condition.
  • domain assumption Boundary representations of bulk modes must have correlators that transform covariantly under boundary dilatations.
    Stated as the natural expectation that motivates the covariance condition.

pith-pipeline@v0.9.0 · 5392 in / 1414 out tokens · 53639 ms · 2026-05-13T18:06:55.246847+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

28 extracted references · 28 canonical work pages

  1. [1]

    S. S. Gubser, Igor R. Klebanov, and A. W. Peet. Entropy and temperature of black 3-branes.Phys. Rev. D, 54:3915–3919, 1996. 7

  2. [2]

    Horowitz and Veronika E

    Gary T. Horowitz and Veronika E. Hubeny. Quasinormal modes of AdS black holes and the approach to thermal equilibrium.Phys. Rev. D, 62:024027, 2000

  3. [3]

    Son, and Andrei O

    Giuseppe Policastro, Dam T. Son, and Andrei O. Starinets. From AdS / CFT correspondence to hydrodynamics. JHEP, 09:043, 2002

  4. [4]

    Son, and Andrei O

    Giuseppe Policastro, Dam T. Son, and Andrei O. Starinets. From AdS / CFT correspondence to hydrodynamics

  5. [5]

    Sound waves.JHEP, 12:054, 2002

  6. [6]

    Son and Andrei O

    Dam T. Son and Andrei O. Starinets. Viscosity, Black Holes, and Quantum Field Theory.Ann. Rev. Nucl. Part. Sci., 57:95–118, 2007

  7. [7]

    Policastro, Dan T

    G. Policastro, Dan T. Son, and Andrei O. Starinets. The Shear viscosity of strongly coupled N=4 supersymmetric Yang-Mills plasma.Phys. Rev. Lett., 87:081601, 2001

  8. [8]

    Kovtun, Dan T

    P. Kovtun, Dan T. Son, and Andrei O. Starinets. Viscosity in strongly interacting quantum field theories from black hole physics.Phys. Rev. Lett., 94:111601, 2005

  9. [9]

    Kovtun and Andrei O

    Pavel K. Kovtun and Andrei O. Starinets. Quasinormal modes and holography.Phys. Rev. D, 72:086009, 2005

  10. [10]

    V. K. Dobrev. Intertwining operator realization of the AdS / CFT correspondence.Nucl. Phys. B, 553:559–582, 1999

  11. [11]

    On the construction of local fields in the bulk of AdS(5) and other spaces.Phys

    Iosif Bena. On the construction of local fields in the bulk of AdS(5) and other spaces.Phys. Rev. D, 62:066007, 2000

  12. [12]

    Kabat, Gilad Lifschytz, and David A

    Alex Hamilton, Daniel N. Kabat, Gilad Lifschytz, and David A. Lowe. Local bulk operators in AdS/CFT: A Boundary view of horizons and locality.Phys. Rev. D, 73:086003, 2006

  13. [13]

    Kabat, Gilad Lifschytz, and David A

    Alex Hamilton, Daniel N. Kabat, Gilad Lifschytz, and David A. Lowe. Holographic representation of local bulk operators.Phys. Rev. D, 74:066009, 2006

  14. [14]

    Lectures on Bulk Reconstruction.SciPost Phys

    Nirmalya Kajuri. Lectures on Bulk Reconstruction.SciPost Phys. Lect. Notes, 22:1, 2021

  15. [15]

    An Infalling Observer in AdS/CFT.JHEP, 10:212, 2013

    Kyriakos Papadodimas and Suvrat Raju. An Infalling Observer in AdS/CFT.JHEP, 10:212, 2013

  16. [16]

    Monica Guica and Simon F. Ross. Behind the geon horizon.Class. Quant. Grav., 32(5):055014, 2015

  17. [17]

    Bulk reconstruction in rotating BTZ black hole.Phys

    Nirmalya Kajuri. Bulk reconstruction in rotating BTZ black hole.Phys. Rev. D, 103(6):066019, 2021

  18. [18]

    Bulk reconstruction in 2D multihorizon black hole.Phys

    Parijat Dey, Nirmalya Kajuri, and Rhitaparna Pal. Bulk reconstruction in 2D multihorizon black hole.Phys. Rev. D, 111(12):126003, 2025

  19. [19]

    State-Dependent Bulk-Boundary Maps and Black Hole Complemen- tarity.Phys

    Kyriakos Papadodimas and Suvrat Raju. State-Dependent Bulk-Boundary Maps and Black Hole Complemen- tarity.Phys. Rev. D, 89(8):086010, 2014

  20. [20]

    Black Hole Interior in the Holographic Correspondence and the Infor- mation Paradox.Phys

    Kyriakos Papadodimas and Suvrat Raju. Black Hole Interior in the Holographic Correspondence and the Infor- mation Paradox.Phys. Rev. Lett., 112(5):051301, 2014

  21. [21]

    Remarks on the necessity and implications of state-dependence in the black hole interior.Phys

    Kyriakos Papadodimas and Suvrat Raju. Remarks on the necessity and implications of state-dependence in the black hole interior.Phys. Rev. D, 93(8):084049, 2016

  22. [22]

    Local Operators in the Eternal Black Hole.Phys

    Kyriakos Papadodimas and Suvrat Raju. Local Operators in the Eternal Black Hole.Phys. Rev. Lett., 115(21):211601, 2015

  23. [23]

    The black hole interior from non-isometric codes and complexity.JHEP, 06:155, 2024

    Chris Akers, Netta Engelhardt, Daniel Harlow, Geoff Penington, and Shreya Vardhan. The black hole interior from non-isometric codes and complexity.JHEP, 06:155, 2024

  24. [24]

    Non-isometric codes for the black hole interior from fundamental and effective dynamics.JHEP, 09:068, 2023

    Oliver DeWolfe and Kenneth Higginbotham. Non-isometric codes for the black hole interior from fundamental and effective dynamics.JHEP, 09:068, 2023

  25. [25]

    Cosmology from random entanglement.JHEP, 11:188, 2023

    Stefano Antonini, Martin Sasieta, and Brian Swingle. Cosmology from random entanglement.JHEP, 11:188, 2023

  26. [26]

    Bulk reconstruction and non-isometry in the backwards-forwards holographic black hole map.JHEP, 06:126, 2024

    Oliver DeWolfe and Kenneth Higginbotham. Bulk reconstruction and non-isometry in the backwards-forwards holographic black hole map.JHEP, 06:126, 2024

  27. [27]

    Non-isometry, state dependence and holography.JHEP, 02:150, 2025

    Stefano Antonini, Vijay Balasubramanian, Ning Bao, ChunJun Cao, and Wissam Chemissany. Non-isometry, state dependence and holography.JHEP, 02:150, 2025

  28. [28]

    Tensor networks for black hole interiors: non-isometries, quantum extremal surfaces, and wormholes.JHEP, 10:012, 2024

    Gracemarie Bueller, Oliver DeWolfe, and Kenneth Higginbotham. Tensor networks for black hole interiors: non-isometries, quantum extremal surfaces, and wormholes.JHEP, 10:012, 2024