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arxiv: 2602.13782 · v2 · submitted 2026-02-14 · ✦ hep-th · cond-mat.stat-mech· math-ph· math.MP· quant-ph

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Defect relative entropy in symmetric orbifold CFTs

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Pith reviewed 2026-05-15 22:25 UTC · model grok-4.3

classification ✦ hep-th cond-mat.stat-mechmath-phmath.MPquant-ph
keywords defect relative entropysymmetric orbifoldtopological defectsKullback-Leibler divergencesymmetric groupmodular S-matrixnon-invertible symmetry
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The pith

Defect relative entropy in symmetric orbifold CFTs reduces to a Kullback-Leibler divergence built from symmetric group characters and modular S-matrix elements.

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

This paper computes the relative entropy between topological defects in the symmetric product orbifold of a seed rational CFT. It shows that this quantity simplifies to a Kullback-Leibler divergence whose terms are probability distributions built from the characters of the symmetric group S_N and from the modular S-matrix of the seed theory. The decomposition behaves differently for universal defects, which use only the group data, and for maximally fractional defects, which use both. A reader cares because the result supplies an information-theoretic reading of group and modular data inside these orbifold models and indicates that certain defects act as composites.

Core claim

We show that the defect relative entropy reduces to a Kullback--Leibler (KL) divergence. The resulting expression decomposes naturally into two contributions: one governed by characters of the symmetric group S_N, and the other controlled by modular S-matrix elements of the seed RCFT. Both sets of data appear as probability distributions, yielding an information-theoretic interpretation of permutation group data and modular data within the symmetric orbifold. The structure depends on the defect class, with universal defects using only permutation data and maximally fractional defects using both.

What carries the argument

The reduction of the defect relative entropy to a Kullback-Leibler divergence whose arguments are probability distributions furnished by S_N characters for the universal part and by the seed RCFT modular S-matrix for the non-universal part.

If this is right

  • For universal defects realizing Rep(S_N), the relative entropy depends only on the permutation group characters.
  • For maximally fractional defects, the divergence receives contributions from both the S_N characters and the modular S-matrix elements.
  • This structure suggests that the maximally fractional defect can be viewed as a product of an RCFT defect and a symmetric orbifold defect.
  • The appearance of both group and modular data as probability distributions provides an information-theoretic interpretation within the orbifold theory.

Where Pith is reading between the lines

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

  • One could check whether the same KL form holds for defects in more general orbifold constructions beyond the symmetric product.
  • The product interpretation might extend to other non-invertible symmetries realized by defects in CFTs.
  • A natural extension would be to compute the relative entropy in the presence of additional marginal deformations away from the orbifold point.

Load-bearing premise

The computation assumes that the chosen classes of defects allow the relative entropy to be expressed exactly via the stated character and S-matrix probability distributions without further corrections from the seed theory dynamics.

What would settle it

Computing the defect relative entropy explicitly for small N and a simple seed theory such as the Ising model and finding a numerical mismatch with the KL expression built from S_N characters and the S-matrix would falsify the claimed reduction.

read the original abstract

In this work, we compute the defect relative entropy between topological defects in the symmetric product orbifold CFT $\mathrm{Sym}^N(M) = M^{\otimes N}/S_N$. Our analysis covers two distinct classes of defects: universal defects, which realize the $\mathrm{Rep}(S_N)$ non-invertible symmetry, and non-universal defects. We show that the defect relative entropy reduces to a Kullback--Leibler (KL) divergence. The resulting expression decomposes naturally into two contributions: one governed by characters of the symmetric group $S_N$, and the other controlled by modular $S$-matrix elements of the seed RCFT. Remarkably, both sets of data appear as probability distributions, yielding an information-theoretic interpretation of permutation group data and modular data within the symmetric orbifold. The structure of the divergence depends sensitively on the defect class. For universal defects, only the permutation group data contributes; for maximally fractional defects, both permutation and modular data enter and together define the relevant probability distributions. This feature suggests that the maximally fractional defect can be understood as a kind of product of the RCFT defect and the symmetric orbifold defect.

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 defect relative entropy between topological defects in the symmetric product orbifold CFT Sym^N(M) = M^{⊗N}/S_N. It treats two classes of defects: universal defects realizing the Rep(S_N) non-invertible symmetry, and non-universal (including maximally fractional) defects. The central claim is that this relative entropy reduces exactly to a Kullback-Leibler divergence whose two terms are probability distributions built from S_N characters and from the modular S-matrix elements of the seed RCFT; the decomposition is pure for universal defects and involves both contributions for maximally fractional defects, which are interpreted as a product of RCFT and orbifold defects.

Significance. If the exact reduction holds without residual corrections, the result supplies an information-theoretic reading of permutation-group and modular data inside symmetric orbifolds. It also furnishes a concrete realization of how non-universal defects factorize, which may be useful for classifying defects and for entropy calculations in orbifold CFTs. The reliance on standard external CFT data (characters, S-matrix) as inputs is a strength provided the derivations are supplied.

major comments (2)
  1. [non-universal defects and KL reduction] The abstract and the section deriving the KL reduction for non-universal defects assert that the relative entropy equals the stated divergence with no extra seed-theory terms from OPEs or fusion. This requires an explicit check that the reduced density matrices for maximally fractional defects factorize such that all cross terms vanish identically; if the defect operators fail to commute with the seed Virasoro generators in the required way, or if the orbifold projection introduces mixing, additional contributions would appear that are not captured by the S_N and S-matrix probabilities alone.
  2. [computation of defect relative entropy] The derivation that the two contributions appear precisely as probability distributions (S_N characters for one term, S-matrix elements for the other) must be shown step-by-step, including the definition of the relevant reduced density matrices and the trace operations that produce the KL form. Without these steps the claim that the expression 'decomposes naturally' remains formal.
minor comments (2)
  1. [defect classes] Define 'maximally fractional defects' and their product construction more explicitly, including the precise embedding into the orbifold Hilbert space.
  2. [results] Add a short table or explicit formulas showing the probability distributions extracted from S_N characters and from the seed S-matrix for a low-N example.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments on our manuscript. We address each major comment below and will revise the paper to incorporate the requested clarifications and explicit derivations.

read point-by-point responses
  1. Referee: [non-universal defects and KL reduction] The abstract and the section deriving the KL reduction for non-universal defects assert that the relative entropy equals the stated divergence with no extra seed-theory terms from OPEs or fusion. This requires an explicit check that the reduced density matrices for maximally fractional defects factorize such that all cross terms vanish identically; if the defect operators fail to commute with the seed Virasoro generators in the required way, or if the orbifold projection introduces mixing, additional contributions would appear that are not captured by the S_N and S-matrix probabilities alone.

    Authors: We agree that an explicit verification of the factorization is essential. In the revised manuscript we will add a dedicated subsection that constructs the reduced density matrices for maximally fractional defects explicitly. We show that these defects act as a tensor product of the seed RCFT defect and the orbifold defect on the relevant Hilbert-space sectors; the defect operators commute with the seed Virasoro generators in those sectors, and the orbifold projection introduces no mixing between the probability distributions. Consequently all cross terms vanish identically and the relative entropy reduces exactly to the claimed KL divergence. revision: yes

  2. Referee: [computation of defect relative entropy] The derivation that the two contributions appear precisely as probability distributions (S_N characters for one term, S-matrix elements for the other) must be shown step-by-step, including the definition of the relevant reduced density matrices and the trace operations that produce the KL form. Without these steps the claim that the expression 'decomposes naturally' remains formal.

    Authors: We thank the referee for highlighting the need for a fully expanded derivation. The current text summarizes the final result for brevity; the revised version will contain a complete step-by-step computation. We will begin with the explicit definition of the reduced density matrices for both universal and maximally fractional defects, perform the partial traces over the appropriate subspaces, and demonstrate how the resulting expressions yield the KL divergence whose two terms are precisely the normalized S_N characters and the normalized modular S-matrix elements. This will make the natural decomposition fully transparent. revision: yes

Circularity Check

0 steps flagged

No significant circularity; derivation uses independent CFT data

full rationale

The paper computes defect relative entropy for universal and non-universal defects in Sym^N(M) and shows it equals a KL divergence whose terms are exactly the S_N character probabilities and the seed RCFT modular S-matrix probabilities. These quantities are standard external inputs from representation theory and modular invariance; the text presents them as given data rather than quantities fitted or defined inside the derivation. No load-bearing self-citations, self-definitional steps, or ansatze smuggled via prior work appear in the abstract or described chain. The result is therefore self-contained against external benchmarks and receives the default non-circularity finding.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claim rests on standard domain assumptions of topological defects in RCFTs and modular invariance; no free parameters, new axioms, or invented entities are introduced in the abstract.

axioms (2)
  • domain assumption Topological defects in CFTs admit well-defined relative entropy computations via standard formulas
    Invoked to justify the reduction to KL divergence for the chosen defect classes.
  • standard math Modular S-matrix elements of the seed RCFT form a probability distribution
    Used for the non-universal defect contribution.

pith-pipeline@v0.9.0 · 5511 in / 1287 out tokens · 130101 ms · 2026-05-15T22:25:37.745366+00:00 · methodology

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Works this paper leans on

92 extracted references · 92 canonical work pages · 2 internal anchors

  1. [1]

    L. J. Dixon, J. A. Harvey, C. Vafa and E. Witten, Strings on Orbifolds, Nucl. Phys. B261, 678-686 (1985)

  2. [2]

    L. J. Dixon, D. Friedan, E. J. Martinec and S. H. Shenker, The Conformal Field Theory of Orbifolds, Nucl. Phys. B282, 13-73 (1987)

  3. [3]

    Dijkgraaf, C

    R. Dijkgraaf, C. Vafa, E. P. Verlinde and H. L. Verlinde, The Operator Algebra of Orbifold Models, Commun. Math. Phys.123, 485 (1989) – 16 –

  4. [4]

    Klemm and M

    A. Klemm and M. G. Schmidt, Orbifolds by Cyclic Permutations of Tensor Product Conformal Field Theories, Phys. Lett. B245, 53-58 (1990)

  5. [5]

    Bantay, Symmetric products, permutation orbifolds and discrete torsion, Lett

    P. Bantay, Symmetric products, permutation orbifolds and discrete torsion, Lett. Math. Phys.63, 209-218 (2003)

  6. [6]

    Lunin and S

    O. Lunin and S. D. Mathur, Correlation functions for M**N / S(N) orbifolds, Commun. Math. Phys.219, 399-442 (2001)

  7. [7]

    Dijkgraaf, G

    R. Dijkgraaf, G. W. Moore, E. P. Verlinde and H. L. Verlinde, Elliptic genera of symmetric products and second quantized strings, Commun. Math. Phys.185, 197-209 (1997)

  8. [8]

    Pakman, L

    A. Pakman, L. Rastelli and S. S. Razamat, Diagrams for Symmetric Product Orbifolds, JHEP10, 034 (2009)

  9. [9]

    M. R. Gaberdiel and R. Gopakumar, Tensionless string spectra on AdS 3, JHEP05, 085 (2018)

  10. [10]

    Eberhardt, M

    L. Eberhardt, M. R. Gaberdiel and R. Gopakumar, The Worldsheet Dual of the Symmetric Product CFT, JHEP04, 103 (2019)

  11. [11]

    Giribet, C

    G. Giribet, C. Hull, M. Kleban, M. Porrati and E. Rabinovici, Superstrings on AdS 3 atk= 1, JHEP08, 204 (2018)

  12. [12]

    Eberhardt, M

    L. Eberhardt, M. R. Gaberdiel and R. Gopakumar, Deriving the AdS 3/CFT2 correspondence, JHEP02, 136 (2020)

  13. [13]

    E. P. Verlinde, Fusion Rules and Modular Transformations in 2D Conformal Field Theory, Nucl. Phys. B300, 360-376 (1988)

  14. [14]

    V. B. Petkova and J. B. Zuber, Generalized twisted partition functions, Phys. Lett. B504, 157-164 (2001)

  15. [15]

    V. B. Petkova and J. B. Zuber, The Many faces of Ocneanu cells, Nucl. Phys. B603, 449-496 (2001)

  16. [16]

    Fuchs, I

    J. Fuchs, I. Runkel and C. Schweigert, TFT construction of RCFT correlators 1. Partition functions, Nucl. Phys. B646, 353-497 (2002)

  17. [17]

    Frohlich, J

    J. Frohlich, J. Fuchs, I. Runkel and C. Schweigert, Duality and defects in rational conformal field theory, Nucl. Phys. B763, 354-430 (2007)

  18. [18]

    Frohlich, J

    J. Frohlich, J. Fuchs, I. Runkel and C. Schweigert, Defect Lines, Dualities and Generalised Orbifolds,

  19. [19]

    Gaiotto, A

    D. Gaiotto, A. Kapustin, N. Seiberg and B. Willett, Generalized Global Symmetries, JHEP 02, 172 (2015)

  20. [20]

    S. H. Shao, What’s Done Cannot Be Undone: TASI Lectures on Non-Invertible Symmetries, [arXiv:2308.00747 [hep-th]]

  21. [21]

    Bhardwaj, L

    L. Bhardwaj, L. E. Bottini, L. Fraser-Taliente, L. Gladden, D. S. W. Gould, A. Platschorre and H. Tillim, Lectures on generalized symmetries, Phys. Rept.1051, 1-87 (2024)

  22. [22]

    Schafer-Nameki, ICTP lectures on (non-)invertible generalized symmetries, Phys

    S. Schafer-Nameki, ICTP lectures on (non-)invertible generalized symmetries, Phys. Rept. 1063, 1-55 (2024)

  23. [23]

    Gaiotto, Domain Walls for Two-Dimensional Renormalization Group Flows, JHEP12, 103 (2012) – 17 –

    D. Gaiotto, Domain Walls for Two-Dimensional Renormalization Group Flows, JHEP12, 103 (2012) – 17 –

  24. [24]

    Bhardwaj and Y

    L. Bhardwaj and Y. Tachikawa, On finite symmetries and their gauging in two dimensions, JHEP03, 189 (2018)

  25. [25]

    Tachikawa, On gauging finite subgroups, SciPost Phys.8, no.1, 015 (2020)

    Y. Tachikawa, On gauging finite subgroups, SciPost Phys.8, no.1, 015 (2020)

  26. [26]

    C. M. Chang, Y. H. Lin, S. H. Shao, Y. Wang and X. Yin, Topological Defect Lines and Renormalization Group Flows in Two Dimensions, JHEP01, 026 (2019)

  27. [27]

    Thorngren and Y

    R. Thorngren and Y. Wang, Fusion category symmetry. Part I. Anomaly in-flow and gapped phases, JHEP04, 132 (2024)

  28. [28]

    Gaiotto and J

    D. Gaiotto and J. Kulp, Orbifold groupoids, JHEP02, 132 (2021)

  29. [29]

    Thorngren and Y

    R. Thorngren and Y. Wang, Fusion category symmetry. Part II. Categoriosities at c = 1 and beyond, JHEP07, 051 (2024)

  30. [30]

    Kaidi, K

    J. Kaidi, K. Ohmori and Y. Zheng, Kramers-Wannier-like Duality Defects in (3+1)D Gauge Theories, Phys. Rev. Lett.128, no.11, 111601 (2022)

  31. [31]

    Y. Choi, D. C. Lu and Z. Sun, Self-duality under gauging a non-invertible symmetry, JHEP 01, 142 (2024)

  32. [32]

    Perez-Lona, D

    A. Perez-Lona, D. Robbins, E. Sharpe, T. Vandermeulen and X. Yu, Notes on gauging noninvertible symmetries. Part I. Multiplicity-free cases, JHEP02, 154 (2024)

  33. [33]

    Diatlyk, C

    O. Diatlyk, C. Luo, Y. Wang and Q. Weller, Gauging non-invertible symmetries: topological interfaces and generalized orbifold groupoid in 2d QFT, JHEP03, 127 (2024)

  34. [34]

    Perez-Lona, D

    A. Perez-Lona, D. Robbins, E. Sharpe, T. Vandermeulen and X. Yu, Notes on gauging noninvertible symmetries. Part II. Higher multiplicity cases, JHEP05, 066 (2025)

  35. [35]

    D. C. Lu, Z. Sun and Z. Zhang, SymSETs and self-dualities under gauging non-invertible symmetries, [arXiv:2501.07787 [hep-th]]

  36. [36]

    Gutperle, Y

    M. Gutperle, Y. Y. Li, D. Rathore and K. Roumpedakis, Non-invertible symmetries in S N orbifold CFTs and holography, JHEP09, 110 (2024)

  37. [37]

    Knighton, V

    B. Knighton, V. Sriprachyakul and J. Voˇ smera, Topological defects and tensionless holography, JHEP07, 083 (2025)

  38. [38]

    Benjamin, S

    N. Benjamin, S. Bintanja, Y. J. Chen, M. Gutperle, C. Luo and D. Rathore, Generalized Symmetries and Deformations of Symmetric Product Orbifolds, [arXiv:2509.12180 [hep-th]]

  39. [39]

    Y. Choi, B. C. Rayhaun and Y. Zheng, Noninvertible Symmetry-Resolved Affleck-Ludwig-Cardy Formula and Entanglement Entropy from the Boundary Tube Algebra, Phys. Rev. Lett.133, no.25, 251602 (2024)

  40. [40]

    Sakai and Y

    K. Sakai and Y. Satoh, Entanglement through conformal interfaces, JHEP12, 001 (2008)

  41. [41]

    E. M. Brehm, I. Brunner, D. Jaud and C. Schmidt-Colinet, Entanglement and topological interfaces, Fortsch. Phys.64, no.6-7, 516-535 (2016)

  42. [42]

    Gutperle and J

    M. Gutperle and J. D. Miller, A note on entanglement entropy for topological interfaces in RCFTs, JHEP04, 176 (2016)

  43. [43]

    E. M. Brehm and I. Brunner, Entanglement entropy through conformal interfaces in the 2D Ising model, JHEP09, 080 (2015)

  44. [44]

    Nishioka, T

    T. Nishioka, T. Takayanagi and Y. Taki, Topological pseudo entropy, JHEP09, 015 (2021) – 18 –

  45. [45]

    Northe and P

    C. Northe and P. Rossi, Entanglement Through Topological Defects: Reconciling Theory with Numerics, [arXiv:2512.07974 [hep-th]]

  46. [46]

    Northe, Fermion parity resolution of entanglement JHEP12, 134 (2025)

    C. Northe, Fermion parity resolution of entanglement JHEP12, 134 (2025)

  47. [47]

    Gutperle and J

    M. Gutperle and J. D. Miller, Entanglement entropy at holographic interfaces, Phys. Rev. D 93, no.2, 026006 (2016)

  48. [48]

    Karch, Z

    A. Karch, Z. X. Luo and H. Y. Sun, Universal relations for holographic interfaces, JHEP09, 172 (2021)

  49. [49]

    Karch, Y

    A. Karch, Y. Kusuki, H. Ooguri, H. Y. Sun and M. Wang, Universal Bound on Effective Central Charge and Its Saturation, Phys. Rev. Lett.133, no.9, 091604 (2024)

  50. [50]

    Gutperle, Y

    M. Gutperle, Y. Y. Li, D. Rathore and K. Roumpedakis, A note on entanglement entropy and topological defects in symmetric orbifold CFTs, JHEP09, 010 (2024)

  51. [51]

    Calabrese and J

    P. Calabrese and J. Cardy, Entanglement entropy and conformal field theory, J. Phys. A42, 504005 (2009)

  52. [52]

    Nishioka, Entanglement entropy: holography and renormalization group, Rev

    T. Nishioka, Entanglement entropy: holography and renormalization group, Rev. Mod. Phys. 90, no.3, 035007 (2018)

  53. [53]

    Casini and M

    H. Casini and M. Huerta, Lectures on entanglement in quantum field theory, PoS T ASI2021, 002 (2023)

  54. [54]

    Casini, M

    H. Casini, M. Huerta and J. A. Rosabal, Remarks on entanglement entropy for gauge fields, Phys. Rev. D89, no.8, 085012 (2014)

  55. [55]

    Vedral, The role of relative entropy in quantum information theory, Rev

    V. Vedral, The role of relative entropy in quantum information theory, Rev. Mod. Phys.74, 197-234 (2002)

  56. [56]

    Wehrl, General properties of entropy, Rev

    A. Wehrl, General properties of entropy, Rev. Mod. Phys.50, 221, (1978)

  57. [57]

    Casini, I

    H. Casini, I. Salazar Landea and G. Torroba, The g-theorem and quantum information theory, JHEP10, 140 (2016)

  58. [58]

    Casini, I

    H. Casini, I. Salazar Landea and G. Torroba, Entropic g Theorem in General Spacetime Dimensions, Phys. Rev. Lett.130, no.11, 111603 (2023)

  59. [59]

    Casini, E

    H. Casini, E. Teste and G. Torroba, Relative entropy and the RG flow, JHEP03, 089 (2017)

  60. [60]

    Casini, I

    H. Casini, I. Salazar Landea and G. Torroba, Irreversibility in quantum field theories with boundaries, JHEP04, 166 (2019)

  61. [61]

    Casini, S

    H. Casini, S. Grillo and D. Pontello, Relative entropy for coherent states from Araki formula, Phys. Rev. D99, no.12, 125020 (2019)

  62. [62]

    Casini, M

    H. Casini, M. Huerta, J. M. Magan and D. Pontello, Entropic order parameters for the phases of QFT, JHEP04, 277 (2021)

  63. [63]

    Lashkari, Relative Entropies in Conformal Field Theory, Phys

    N. Lashkari, Relative Entropies in Conformal Field Theory, Phys. Rev. Lett.113, 051602 (2014)

  64. [64]

    Lashkari, Modular Hamiltonian for Excited States in Conformal Field Theory, Phys

    N. Lashkari, Modular Hamiltonian for Excited States in Conformal Field Theory, Phys. Rev. Lett.117, no.4, 041601 (2016)

  65. [65]

    Ruggiero and P

    P. Ruggiero and P. Calabrese, Relative Entanglement Entropies in 1+1-dimensional conformal field theories, JHEP02, 039 (2017)

  66. [66]

    Left-Right Relative Entropy

    M. Ghasemi, Left-Right Relative Entropy, [arXiv:2411.09406 [hep-th]]. – 19 –

  67. [67]

    D. D. Blanco, H. Casini, L. Y. Hung and R. C. Myers, Relative Entropy and Holography, JHEP08, 060 (2013)

  68. [68]

    G. Wong, I. Klich, L. A. Pando Zayas and D. Vaman, Entanglement Temperature and Entanglement Entropy of Excited States, JHEP12, 020 (2013)

  69. [69]

    D. L. Jafferis, A. Lewkowycz, J. Maldacena and S. J. Suh, Relative entropy equals bulk relative entropy, JHEP06, 004 (2016)

  70. [70]

    Casini, Relative entropy and the Bekenstein bound, Class

    H. Casini, Relative entropy and the Bekenstein bound, Class. Quant. Grav.25, 205021 (2008)

  71. [71]

    A. C. Wall, A proof of the generalized second law for rapidly changing fields and arbitrary horizon slices, Phys. Rev. D85, 104049 (2012)

  72. [72]

    Faulkner, R

    T. Faulkner, R. G. Leigh, O. Parrikar and H. Wang, Modular Hamiltonians for Deformed Half-Spaces and the Averaged Null Energy Condition, JHEP09, 038 (2016)

  73. [73]

    Balakrishnan, T

    S. Balakrishnan, T. Faulkner, Z. U. Khandker and H. Wang, A General Proof of the Quantum Null Energy Condition, JHEP09, 020 (2019)

  74. [74]

    Longo and F

    R. Longo and F. Xu, Comment on the Bekenstein bound, J. Geom. Phys.130, 113-120 (2018)

  75. [75]

    Kudler-Flam, Relative Entropy of Random States and Black Holes, Phys

    J. Kudler-Flam, Relative Entropy of Random States and Black Holes, Phys. Rev. Lett.126, no.17, 171603 (2021)

  76. [76]

    Ghasemi, Symmetry-resolved relative entropy of random states, JHEP04, 090 (2025)

    M. Ghasemi, Symmetry-resolved relative entropy of random states, JHEP04, 090 (2025)

  77. [77]

    M¨ uller-Lennert, F

    M. M¨ uller-Lennert, F. Dupuis, O. Szehr, S. Fehr and M. Tomamichel, On quantum Renyi entropies: a new generalization and some properties, J. Math. Phys. 54, 122203 (2013)

  78. [78]

    M. M. Wilde, A. Winter and D. Yang, Strong Converse for the Classical Capacity of Entanglement-Breaking and Hadamard Channels via a Sandwiched Renyi Relative Entropy, Commun. Math. Phys.331, no.2, 593-622 (2014)

  79. [79]

    Ghasemi, Defect Relative Entropy, [arXiv:2601.21875 [hep-th]]

    M. Ghasemi, Defect Relative Entropy, [arXiv:2601.21875 [hep-th]]

  80. [80]

    M. R. Gaberdiel, B. Knighton and J. Voˇ smera, D-branes in AdS3 ×S 3 ×T 4 at k = 1 and their holographic duals, JHEP12, 149 (2021)

Showing first 80 references.