{"total":13,"items":[{"citing_arxiv_id":"2606.30853","ref_index":122,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Rethinking quantum information in gravity and fields","primary_cat":"hep-th","submitted_at":"2026-06-29T19:34:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"The paper organizes important open questions in quantum gravity and quantum information into four themes without presenting new results or derivations.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.22810","ref_index":56,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"A Linearized Obstruction to the Supersymmetric Extension of Conformal Boundary Conditions in Euclidean Gravity","primary_cat":"hep-th","submitted_at":"2026-06-22T03:39:57+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Witten's conformal boundary condition admits no half-supersymmetric extension in linearized minimal supergravity because supersymmetry maps the natural gravitino datum to the trace-free extrinsic curvature left unfixed by the conformal prescription.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.28958","ref_index":33,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Quantum State of a Gravitating Region","primary_cat":"hep-th","submitted_at":"2026-05-27T18:02:11+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Proposal that compact d-manifolds with elliptic data prepare boundary quantum states |J>, with Rényi entropies from path integrals agreeing with minimal-surface formulas after analytic continuation.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.28753","ref_index":13,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"GR from RG, $2d$ Example: JT-Gravity Induced from Renormalization Group Flow","primary_cat":"hep-th","submitted_at":"2026-05-27T17:12:13+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Holographic RG flow on a 2D CFT induces JT gravity with bulk lapse as dilaton and recovers TTbar deformation in the Fefferman-Graham limit.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.23387","ref_index":17,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Probing deformations","primary_cat":"hep-th","submitted_at":"2026-05-22T08:58:55+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Poly-vector deformations of Type II and 11D backgrounds induce TTbar-like flows on the world-volume theories of strings and branes for both abelian and non-abelian deformations.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.13956","ref_index":135,"ref_count":2,"confidence":0.98,"is_internal_anchor":true,"paper_title":"q-Askey Deformations of Double-Scaled SYK","primary_cat":"hep-th","submitted_at":"2026-05-13T18:00:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"q-Askey deformations of DSSYK produce transfer matrices from basic orthogonal polynomials whose chord numbers map to ER bridge lengths and signal geometric transitions with discrete spectra in sine dilaton gravity.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"with negative length, and it has equivalent effects as opening an eternal traversable wormhole - 7 - due to negative energy matter in AdS2. We also relate our results to Cauchy slice holography [128-132], where one finds a tran- sition between Euclidean and Lorentzian geometries by increasing the TT deformation pa- rameter [133, 134] in higher-dimensional finite cutoff holography [135, 136]. Thus, the ETW brane parameter in sine dilaton gravity, which is controlled by the deformation parameter in our setting, acts analogously to the radial cutoff in Cauchy slice holography. In our case, the energy spectrum varies discretely along the flow induced by the deformation parameter instead of continuously for TT deformations. In Sec. 4, we discuss the operator algebras of the deformed theories, particularly, we"},{"citing_arxiv_id":"2605.12616","ref_index":11,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Butterflies in $\\textrm{T}\\overline{\\textrm{T}}$ deformed anomalous CFT$_2$","primary_cat":"hep-th","submitted_at":"2026-05-12T18:05:29+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"In TTbar-deformed anomalous CFT2 the chaos bound stays saturated while butterfly velocity depends nontrivially on deformation strength and anomaly, with a Hagedorn regime where the chaotic response turns complex.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Kutasov,Holography Beyond AdS,Nucl. Phys. B 932(2018) 241-253, [1711.02690]. [9] V. Shyam,Background independent holographic dual toT¯Tdeformed CFT with large central charge in 2 dimensions,JHEP10(2017) 108, [1707.08118]. - 37 - [10] W. Cottrell and A. Hashimoto,Comments onT ¯Tdouble trace deformations and boundary conditions,Phys. Lett. B789(2019) 251-255, [1801.09708]. [11] T. Hartman, J. Kruthoff, E. Shaghoulian and A. Tajdini,Holography at finite cutoff with a T 2 deformation,JHEP03(2019) 004, [1807.11401]. [12] V. Shyam,Finite Cutoff AdS5 Holography and the Generalized Gradient Flow,JHEP12 (2018) 086, [1808.07760]. [13] G. Jafari, A. Naseh and H. Zolfi,Path Integral Optimization forT¯TDeformation,Phys. Rev. D101(2020) 026007, [1909."},{"citing_arxiv_id":"2604.10267","ref_index":48,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"The yes boundaries wavefunctions of the universe","primary_cat":"hep-th","submitted_at":"2026-04-11T16:09:43+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Using two timelike boundaries and a nearly maximally entangled thermofield double state from dressed de Sitter Hamiltonian theories, the authors construct wavefunctions for extended cosmological spacetimes that include the future wedge and resolve entanglement entropy issues via 3D constrained path ","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Verlinde, Moving the CFT into the bulk withT T, JHEP04(2018) 010 [1611.03470]. [45] P. Kraus, J. Liu and D. Marolf, Cutoff AdS3 versus theT Tdeformation, JHEP07(2018) 027 [1801.02714]. [46] M. Guica and R. Monten, T ¯Tand the mirage of a bulk cutoff,1906.11251. [47] V. Gorbenko, E. Silverstein and G. Torroba, dS/dS andT T, JHEP03(2019) 085 [1811.07965]. [48] T. Hartman, J. Kruthoff, E. Shaghoulian and A. Tajdini, Holography at finite cutoff with a t2 deformation, JHEP03(2019) 004 [1807.11401]. [49] D.J. Gross, J. Kruthoff, A. Rolph and E. Shaghoulian, T Tin AdS 2 and Quantum Mechanics, 1907.04873. [50] K. Allameh and E. Shaghoulian, Timelike Liouville theory and AdS 3 gravity at finite cutoff, 2508.03236."},{"citing_arxiv_id":"2604.02514","ref_index":16,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Holographic Banners","primary_cat":"hep-th","submitted_at":"2026-04-02T21:16:13+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"Holographic banners are four-argument on-shell actions that map thermofield double boundary states to future interior semiclassical states and yield BKL mixing timescales in AdS black holes.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Polchinski, Holographic and Wilsonian Renormalization Groups, JHEP06, 031, 2011, [arXiv:1010.1264 [hep-th]]. [14] T. Faulkner, H. Liu and M. Rangamani, Integrating out geometry: Holographic Wilsonian RG and the membrane paradigm, JHEP08, 051, 2011, [arXiv:1010.4036 [hep-th]]. [15] L. McGough, M. Mezei and H. Verlinde, Moving the CFT into the bulk withTT, JHEP04, 010, 2018, [arXiv:1611.03470 [hep-th]]. [16] T. Hartman, J. Kruthoff, E. Shaghoulian and A. Tajdini, Holography at finite cutoff with aT 2 deformation, JHEP03, 004, 2019, [arXiv:1807.11401 [hep-th]]. 31 [17] M. J. Blacker and S. Ning, Wheeler DeWitt states of a charged AdS4 black hole, JHEP12, 002, 2023, [arXiv:2308.00040 [hep-th]]. [18] M. J. Blacker and S. A. Hartnoll, Cosmological quantum states of de"},{"citing_arxiv_id":"2602.11806","ref_index":24,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"GR from RG: Gravity Is Induced From Renormalization Group Flow In The Infrared","primary_cat":"hep-th","submitted_at":"2026-02-12T10:38:42+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Holographic RG flow induces gravity by evolving boundary conditions from rigid Dirichlet to mixed Dirichlet-Neumann, generating an Einstein-Hilbert term and evading the Weinberg-Witten theorem.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2602.06113","ref_index":27,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Deforming the Double-Scaled SYK & Reaching the Stretched Horizon From Finite Cutoff Holography","primary_cat":"hep-th","submitted_at":"2026-02-05T19:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Deformations of the double-scaled SYK model via finite-cutoff holography produce Krylov complexity as wormhole length and realize Susskind's stretched horizon proposal through targeted T² deformations in the high-energy spectrum.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"restriction in deriving the flow equation below, since we investigate cases whereΦB is a finite - 7 - cutoff, instead of a radial regulator of the asymptotic boundary.8 Also, note that in the following one may allowgµνandΦ∈C; which is the case of interest for sine dilaton gravity at finite cutoff. We will discuss this case in detail in App. C. The strategy proposed in [27] is to recover theT2 flow equation from the HJ equation controlling radial evolution along the flow.9 For this reason, we will consider the dilaton- gravity theory as the input for defining the deformed DSSYK model.10 Note that while we implement a similar strategy as [27, 32] to define the Hamiltonian deformations in the boundary theory, the crucial difference with previous approaches in the derivation of the flow"},{"citing_arxiv_id":"2510.10519","ref_index":73,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Integrability in Three-Dimensional Gravity: Eigenfunction-Forced KdV Flows","primary_cat":"hep-th","submitted_at":"2025-10-12T09:35:54+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Derives forced KdV equation from Chern-Simons 3D gravity with chiral boundaries, with forcing set by Schrödinger eigenfunctions, and solves reflectionless and radiative sectors via inverse scattering.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2508.03236","ref_index":22,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Timelike Liouville theory and AdS$_3$ gravity at finite cutoff","primary_cat":"hep-th","submitted_at":"2025-08-05T09:05:10+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Proposes that AdS3 gravity at finite cutoff is dual to a CFT2 coupled to timelike Liouville theory deformed by a marginal operator, with checks via semiclassical partition functions and EOM matching.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}