{"total":13,"items":[{"citing_arxiv_id":"2606.31901","ref_index":26,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Exact Planar Black Hole in AdS-Einstein-Scalar Gravity with IR Emergent Nearly Conformal Fluid","primary_cat":"hep-th","submitted_at":"2026-06-30T16:07:36+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"An exact two-parameter analytic solution for a hairy black brane is derived in AdS-Einstein-scalar gravity, with thermodynamics obeying a generalized first law and Euler relation, and the boundary theory recovering nearly conformal fluid behavior in the IR thermal limit.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.30853","ref_index":115,"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":1,"top_context_role":"background","top_context_polarity":"background","context_text":"[112] N. Lashkari,Entanglement at a Scale and Renormalization Monotones,JHEP01(2019) 219 [1704.05077]. [113] T. Nishioka,Entanglement entropy: holography and renormalization group,Rev. Mod. Phys.90 (2018) 035007 [1801.10352]. [114] M. Bianchi, D.Z. Freedman and K. Skenderis,Holographic renormalization,Nucl. Phys. B631 (2002) 159 [hep-th/0112119]. [115] J. de Boer, E.P. Verlinde and H.L. Verlinde,On the holographic renormalization group,JHEP08 (2000) 003 [hep-th/9912012]. [116] I. Heemskerk and J. Polchinski,Holographic and Wilsonian Renormalization Groups,JHEP06 (2011) 031 [1010.1264]. [117] E. Kiritsis, W. Li and F. Nitti,Holographic RG flow and the Quantum Effective Action,Fortsch. Phys.62(2014) 389 [1401."},{"citing_arxiv_id":"2606.26163","ref_index":14,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Large-$N$ Carrollian Thermodynamics from AdS Black-Hole Phase-Space Contractions","primary_cat":"hep-th","submitted_at":"2026-06-24T06:24:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Finite Carrollian black-hole thermodynamics arises as a double-scaled low-temperature large-N ensemble in AdS/CFT, with the boundary Brown-York stress tensor reproducing the contracted bulk Hamiltonian and first law.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.28753","ref_index":26,"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":"2605.18942","ref_index":6,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Covariant unification of holographic c-functions","primary_cat":"hep-th","submitted_at":"2026-05-18T18:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"A new covariant c-function is defined from extrinsic curvature of codimension-two bulk slices, unifying prior foliation-based definitions and exhibiting expected monotonic behavior in conformal, confining, and mixed-geometry string backgrounds.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Extending this idea to higher dimensions has proven consider- ably more subtle [2-5]. Holography has played a significant role in advancing the subject: in the AdS/CFT correspondence an RG flow is represented as a higher-dimensional spacetime whose ra- dial direction encodes the energy scale, and c-theorems become geometric statements about the bulk [6]. Early holographic proposals for candidate measures of degrees of freedom, so-called c-functions, focused largely on energy conditions, especially the null energy condition (NEC) in gravity [7]. The NEC often ensures the monotonicity of various geometric quantities that underlie many construc- tions of classical holographic c-functions in both bottom-up and top-down settings."},{"citing_arxiv_id":"2605.17209","ref_index":13,"ref_count":2,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Emergent $\\text{AdS}_{d+1}$ Geometry from Functional Renormalization Group in the Massless Critical Limit","primary_cat":"hep-th","submitted_at":"2026-05-17T00:59:46+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Functional renormalization group flow of the O(N) vector model produces an emergent AdS_{d+1} geometry under the massless critical condition.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.10548","ref_index":34,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Birth of Inflationary Universes via Wineglass Wormholes and their No-Boundary Relatives","primary_cat":"hep-th","submitted_at":"2026-05-11T13:26:33+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Wineglass wormholes with a local maximum in the scale factor mediate the birth of inflationary spacetimes and split into background plus no-boundary geometries at small axionic or magnetic charge.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":",\"Phys. Rev. D66 (2002) 123509,arXiv:hep-th/0204212. [32] V. Balasubramanian, P. Kraus, and A. E. Lawrence, \"Bulk versus boundary dynamics in anti-de Sitter space-time,\"Phys. Rev. D59(1999) 046003,arXiv:hep-th/9805171. [33] J. de Boer, E. P. Verlinde, and H. L. Verlinde, \"On the holographic renormalization group,\"JHEP 08(2000) 003,arXiv:hep-th/9912012. [34] H. Elvang and M. Hadjiantonis, \"A Practical Approach to the Hamilton-Jacobi Formulation of Holographic Renormalization,\"JHEP06(2016) 046,arXiv:1603.04485 [hep-th]. [35] D. Marolf and J. E. Santos, \"AdS Euclidean wormholes,\"Class. Quant. Grav.38no. 22, (2021) 224002,arXiv:2101.08875 [hep-th]. [36] G. W. Lyons, \"Complex solutions for the scalar field model of the universe,\"Phys."},{"citing_arxiv_id":"2604.02514","ref_index":11,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"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":"support","context_text":"singularities and the emergence of time, 2022, [arXiv:2211.16512 [hep-th]]. [8] S. Leutheusser and H. Liu, Volume as an index of a subalgebra, 2025, [arXiv:2508.00056 [hep-th]]. [9] S. A. Hartnoll, Wheeler-DeWitt states of the AdS-Schwarzschild interior, JHEP01, 066, 2023, [arXiv:2208.04348 [hep-th]]. [10] B. S. DeWitt, Quantum Theory of Gravity. 1. The Canonical Theory, Phys. Rev.160, 1113-1148, 1967. [11] J. de Boer, E. P. Verlinde and H. L. Verlinde, On the holographic renormalization group, JHEP08, 003, 2000, [arXiv:hep-th/9912012]. [12] S. de Haro, S. N. Solodukhin and K. Skenderis, Holographic reconstruction of space-time and renormalization in the AdS / CFT correspondence, Commun. Math. Phys.217, 595-622, 2001, [arXiv:hep-th/0002230]. [13] I. Heemskerk and J."},{"citing_arxiv_id":"2603.27824","ref_index":52,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Holographic duality from a four-fermion interaction: emergent AdS$_3$/CFT$_2$, D-branes, and Einstein gravity","primary_cat":"hep-th","submitted_at":"2026-03-29T19:30:47+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"The bosonic AdS3/CFT2 duality emerges from the Gross-Neveu model via higher-spin composites and fluctuations in competing spin-0 and spin-1 condensates that define the radial bulk coordinate.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"whereµis a Lagrange multiplier enforcing R dz ρ=N. In the simplest case of species distributed uniformly,ρ(z) =N/z max, the bulk measure is flat and the action reduces to Sbulk = N zmax Z zmax 0 dz Z d2xL ′ Φ1(t, x, z),(2.30) which is manifestly a (2 + 1)-dimensional bulk action with a uniform warp factorN/z max. More generally,ρ(z) encodes the holographic RG flow [52, 53]: it is the bulk density of states as a function of depth, withρ(z)→0 near the boundary (z→0, chiral fixed point) andρ(z) large deep in the bulk (z≫0, classical phase). The saddle-point equation eq. (2.29) is the Callan-Symanzik equation of the boundary RG flow rewritten as a bulk equation for the species density, making the holographic RG interpretation precise [52]."},{"citing_arxiv_id":"2602.11806","ref_index":20,"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":"2601.15878","ref_index":35,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"The thermal backreaction of a scalar field in de Sitter spacetime. II. Spectrum enhancement and holography","primary_cat":"hep-th","submitted_at":"2026-01-22T11:38:11+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Thermal backreaction modifies de Sitter geometry so that late-exiting modes produce a blue-tilted spectrum n_S ~ 2 while the boundary theory matches the 3d Sp(N) model flow.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2311.00550","ref_index":28,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Holographic renormalization and the variational problem for mixed boundary conditions via a solution-dependent superpotential-like function","primary_cat":"hep-th","submitted_at":"2023-11-01T14:33:23+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"For m²L²=-2 in AdS black holes with integrable mixed boundary conditions, the cubic coefficient in the near-boundary expansion of the solution-dependent W(φ) is fixed by the boundary deformation to ensure a well-posed variational principle and finite renormalized action.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2105.14690","ref_index":4,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Holographic $SO(2,d)$ anomaly","primary_cat":"hep-th","submitted_at":"2021-05-31T04:01:54+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"The authors establish the descendant structure of the holographic SO(2,d) anomaly and construct the associated characteristic class, bulk Chern-Simons-like action, boundary effective action, and anomalous conservation laws in covariant and consistent forms.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}