{"total":17,"items":[{"citing_arxiv_id":"2605.23670","ref_index":8,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Twirled Perfect Tensor Networks: Computationally covariant holographic tensor networks","primary_cat":"hep-th","submitted_at":"2026-05-22T14:18:32+00:00","verdict":null,"verdict_confidence":null,"novelty_score":null,"formal_verification":null,"one_line_summary":null,"context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.16641","ref_index":84,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"On bulk reconstruction in Lorentzian AdS and its flat space limit","primary_cat":"hep-th","submitted_at":"2026-05-15T21:31:11+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Constructs bulk scalar field representations in Lorentzian AdS4 from boundary primaries via time-ordered propagators and derives their flat-space limits to plane-wave or Carrollian bases.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"where the bulk-to-boundary propagators are replaced by wavefunctions with respect to an so(3, 1) subalgebra of the AdS4 isometry algebra. The latter will be constructed in Section 6. For simplicity, we will restrict to the case of 4-dimensional spacetimes ( d= 3), but the analysis can be easily generalized to any d. It will be very interesting to revisit ideas building on the HKLL proposal such as entanglement wedge reconstruction [84,103,104], as well as bulk reconstruction in more general backgrounds [82,105] in the light of our results. We hope that the precise relation between the AdS and flat space bulk reconstruction established here in a very simple case will allow us to generalize these interesting features of AdS/CFT to asymptotically flat spacetimes. 17 3 Bulk inner products of AdS bulk-to-boundary propagators"},{"citing_arxiv_id":"2605.13576","ref_index":46,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Semiclassical algebraic reconstruction for type III algebras","primary_cat":"hep-th","submitted_at":"2026-05-13T14:10:23+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Semiclassical crossed product constructions extend the algebraic reconstruction theorem to type III algebras and yield an algebraic Ryu-Takayanagi formula for holographic duality.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"˜ρa in the entanglement wedgea, andL A is the area of the Ryu-Takayanagi surface ofA over4G. The RT formula is so essential that in the holographic framework, the formula - 1 - itself is equivalent to the following three statements according to a series of works [45-47]1, which we call the reconstruction theorem: •Entanglement wedge reconstruction (or subregion duality) [46, 52-60], establishes a correspondence between a boundary subregion and its bulk entanglement wedge, where any bulk operator contained within the entanglement wedge can be recon- structed from information residing on the designated boundary subregion; •The Jafferis-Lewkowycz-Maldacena-Suh (JLMS) formula [60] establishes a duality between boundary and bulk descriptions of quantum information."},{"citing_arxiv_id":"2605.06780","ref_index":53,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"A Semiclassical Diagnostic for Spacetime Emergence","primary_cat":"hep-th","submitted_at":"2026-05-07T18:00:02+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Evanescent quantum extremal surfaces, bounded in area but not generalized entropy, diagnose failures of spacetime emergence in holography.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"6-7 551-564, [arXiv:1604.02589]. [50] L. Susskind and Y. Zhao,Teleportation through the wormhole,Phys. Rev. D98(2018), no. 4 046016, [arXiv:1707.04354]. [51] L. Susskind,Dear Qubitzers, GR =QM,arXiv:1708.03040. [52] B. Czech, J. L. Karczmarek, F. Nogueira, and M. Van Raamsdonk,The Gravity Dual of a Density Matrix,Class.Quant.Grav.29(2012) 155009, [arXiv:1204.1330]. [53] X. Dong, D. Harlow, and A. C. Wall,Reconstruction of Bulk Operators within the Entanglement Wedge in Gauge-Gravity Duality,Phys. Rev. Lett.117(2016), no. 2 021601, [arXiv:1601.05416]. [54] N. Engelhardt and ˚A. Folkestad,Canonical purification of evaporating black holes, Phys. Rev. D105(2022), no. 8 086010, [arXiv:2201.08395]. [55] G. Penington,Entanglement Wedge Reconstruction and the Information Paradox,"},{"citing_arxiv_id":"2604.22612","ref_index":30,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Generalized Entanglement Wedges and the Connected Wedge Theorem","primary_cat":"hep-th","submitted_at":"2026-04-24T14:36:58+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Generalized entanglement wedges rephrase the connected wedge theorem in bulk entropy terms, yielding mutual information bounds and a scattering-to-connected-wedge implication that extends to flat spacetimes.","context_count":1,"top_context_role":"background","top_context_polarity":"support","context_text":"whereE ˆA is the surface homologous to ˆAwhich extremizes the generalized entropy: Sgen(X) := area (X) 4GN +S(a X ) + counterterms.(2.13) HereS( ˆA) is the von Neumann entropy of the boundary region ˆA, whileS(a X ) is the von Neumann entropy of the bulk fields. When the QES prescription holds, it can be shown that the bulk matter inside the associated entanglement wedge is encoded in the boundary state in ˆA[30], in the sense that bulk operators ine W ( ˆA) can be reconstructed from operators in ˆA. The bulk entropy term would nominally seem like a small correction in the semi- classical regime, since the area term isO(1/G N). However, it can be important in the context of black hole evaporation [31-33]. Indeed the entanglement island story mo- tivates more generally analyzing regimes where bulk entropy is significant."},{"citing_arxiv_id":"2604.20165","ref_index":24,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Entropy bound and the non-universality of entanglement islands","primary_cat":"hep-th","submitted_at":"2026-04-22T04:10:59+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Universal compact entanglement islands are obstructed by an entropy bound violation, implying region-dependent interior reconstruction.","context_count":1,"top_context_role":"background","top_context_polarity":"unclear","context_text":"Centre de Physique Th' eorique - X -'Ecole polytechnique - IP Paris - Institut Polytechnique de Paris - CNRS - Centre National de la Recherche Scientifique, Institut polytechnique de Paris, 2025. arXiv:2510.15787 [hep-th]. [23] A. Almheiri, X. Dong, and D. Harlow, \"Bulk Locality and Quantum Error Correction in AdS/CFT,\"JHEP 04(2015) 163,arXiv:1411.7041 [hep-th]. [24] X. Dong, D. Harlow, and A. C. Wall, \"Reconstruction of Bulk Operators within the Entanglement Wedge in Gauge-Gravity Duality,\"Phys. Rev. Lett.117no. 2, (2016) 021601,arXiv:1601.05416 [hep-th]. [25] H. Geng, A. Karch, C. Perez-Pardavila, S. Raju, L. Randall, M. Riojas, and S. Shashi, \"Information Transfer with a Gravitating Bath,\"SciPost Phys.10 no."},{"citing_arxiv_id":"2604.14638","ref_index":87,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Probing bulk geometry via pole skipping: from static to rotating spacetimes","primary_cat":"gr-qc","submitted_at":"2026-04-16T05:28:10+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Pole-skipping data encodes enough information to reconstruct the full metric of 3D rotating black holes and the radial functions of 4D separable rotating black holes, with Einstein equations becoming algebraic constraints on that data.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Hashimoto,Building bulk from Wilson loops,PTEP2021(2021) 023B04 [2008.10883]. [85] D. Kabat and G. Lifschytz,Emergence of spacetime from the algebra of total modular Hamiltonians,JHEP05(2019) 017 [1812.02915]. [86] A. Hamilton, D.N. Kabat, G. Lifschytz and D.A. Lowe,Local bulk operators in AdS/CFT: A Boundary view of horizons and locality,Phys. Rev. D73(2006) 086003 [hep-th/0506118]. [87] X. Dong, D. Harlow and A.C. Wall,Reconstruction of Bulk Operators within the Entanglement Wedge in Gauge-Gravity Duality,Phys. Rev. Lett.117(2016) 021601 [1601.05416]. [88] B. Swingle,Entanglement Renormalization and Holography,Phys. Rev. D86(2012) 065007 [0905.1317]. [89] F. Pastawski, B. Yoshida, D. Harlow and J. Preskill,Holographic quantum error-correcting"},{"citing_arxiv_id":"2512.19452","ref_index":14,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Holographic Tensor Networks as Tessellations of Geometry","primary_cat":"hep-th","submitted_at":"2025-12-22T14:57:18+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Holographic tensor networks constructed from PEE-thread tessellations of AdS geometry reproduce the exact Ryu-Takayanagi formula in factorized EPR, perfect-tensor, and random variants.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2512.11754","ref_index":8,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Modular Witten Diagrams and Quantum Extremality","primary_cat":"hep-th","submitted_at":"2025-12-12T18:05:09+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Modular Witten diagrams reproduce the O(λ² G_N) correction to holographic entanglement entropy, matching the canonical energy term in the quantum Ryu-Takayanagi formula with wedge shape deformation.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.13549","ref_index":8,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Precision tests of bulk entanglement: $AdS_3$ vectors","primary_cat":"hep-th","submitted_at":"2025-11-17T16:19:22+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Bulk single-particle states of a massive Chern-Simons vector in AdS3 produce entanglement entropy corrections that match the CFT replica-trick result for the corresponding primary and descendants at leading and sub-leading orders, with vanishing edge-mode contribution.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.02903","ref_index":56,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Entanglement inequalities, black holes and the architecture of typical states","primary_cat":"hep-th","submitted_at":"2025-11-04T19:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Typical states in large-N holographic CFTs exhibit UV and IR length scales set by energy and charges, producing factorization that isolates black holes via a corona of saturated entanglement wedges and extends ETH to rotating ensembles.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2510.20902","ref_index":74,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Searching for emergent spacetime in spin glasses","primary_cat":"hep-th","submitted_at":"2025-10-23T18:00:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Spectral functions of SYK, p-spin, and SU(M) Heisenberg models show exponential tails in spin-glass phases and quasiparticle families in spin-liquid phases, with a proof that exponential decay blocks detection of bulk causal structure.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2508.00060","ref_index":6,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Entanglement spreading and emergent locality in Brownian SYK chains","primary_cat":"hep-th","submitted_at":"2025-07-31T18:00:02+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"In a Brownian SYK chain at strong coupling, information from an injected qudit spreads inside a sharp light-cone at the butterfly velocity because the governing dynamics reduce to FKPP domain walls.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2309.04231","ref_index":7,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Subregion Complementarity in AdS/CFT","primary_cat":"hep-th","submitted_at":"2023-09-08T09:36:30+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Subregion duality fails in AdS/CFT at leading large N, leading to the proposal of subregion complementarity allowing different CFT operators to describe one bulk subregion.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"1911.12333","ref_index":53,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Replica Wormholes and the Entropy of Hawking Radiation","primary_cat":"hep-th","submitted_at":"2019-11-27T18:23:34+00:00","verdict":"ACCEPT","verdict_confidence":"HIGH","novelty_score":8.0,"formal_verification":"none","one_line_summary":"Replica wormholes in the gravitational path integral yield the island rule for the fine-grained entropy of Hawking radiation, ensuring it follows the unitary Page curve in two-dimensional dilaton gravity.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"1911.11977","ref_index":38,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Replica wormholes and the black hole interior","primary_cat":"hep-th","submitted_at":"2019-11-27T06:30:56+00:00","verdict":"CONDITIONAL","verdict_confidence":"MODERATE","novelty_score":9.0,"formal_verification":"none","one_line_summary":"Replica wormhole geometries justify the replica trick computation of the Page curve in holographic black hole models and support entanglement wedge reconstruction via the Petz map.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"1905.08762","ref_index":8,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"The entropy of bulk quantum fields and the entanglement wedge of an evaporating black hole","primary_cat":"hep-th","submitted_at":"2019-05-21T17:27:30+00:00","verdict":"CONDITIONAL","verdict_confidence":"MODERATE","novelty_score":7.0,"formal_verification":"none","one_line_summary":"In a 2d evaporating black hole model, large boosts create O(1/G_N) gradients in bulk entropy that move the quantum extremal surface, causing the generalized entropy to follow unitary expectations with information disappearing after a scrambling time and a phase transition at the Page time.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}