{"total":153,"items":[{"citing_arxiv_id":"2606.26598","ref_index":12,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Holographic light-quark energy loss in a spinning plasma","primary_cat":"hep-ph","submitted_at":"2026-06-25T04:55:03+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Holographic calculation in a spinning Myers-Perry black brane shows that higher temperature or rotation parameter a shortens light-quark stopping distance and increases instantaneous energy loss, with stronger anisotropy for transverse motion.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.24382","ref_index":4,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Exact and Finite de Sitter QFT from CFT","primary_cat":"hep-th","submitted_at":"2026-06-23T10:15:12+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Constructs exact finite de Sitter QFT from CFT data using moduli space of oriented balls and Casimir completion of operators.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.23522","ref_index":62,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Microscopic entropy of de Sitter spacetime and entropic solution to the old cosmological constant problem","primary_cat":"hep-th","submitted_at":"2026-06-22T16:06:16+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Requiring the RG flow of the de Sitter entropy parameter α to increase monotonically toward the infrared yields a cosmological constant matching the observed value.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.05583","ref_index":6,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Pion structure in Holographic QCD","primary_cat":"hep-ph","submitted_at":"2026-06-04T01:57:59+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"A holographic model with effective linear confinement and gluon condensation simultaneously reproduces the pion mass spectrum and form factors in reasonable agreement with experiment and lattice QCD.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.28958","ref_index":5,"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":23,"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":"2605.28029","ref_index":18,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Embedding formalism for anti-de Sitter superspaces","primary_cat":"hep-th","submitted_at":"2026-05-27T06:35:38+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Develops bi-supertwistor realizations and extensions for N-extended AdS superspaces in 4D/5D with supergravity correspondence and superparticle applications.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.23834","ref_index":25,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Thermodynamics and transport in holographic QCD with Gauss-Bonnet corrections","primary_cat":"hep-th","submitted_at":"2026-05-22T16:42:50+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"A holographic QCD model with dilaton-dependent Gauss-Bonnet corrections matches lattice thermodynamics and yields non-monotonic η/s plus a critical endpoint.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.21252","ref_index":3,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Exact Holographic Kinematics in AdS/CFT","primary_cat":"hep-th","submitted_at":"2026-05-20T14:41:16+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Proposes an exact kinematic sector in AdS/CFT using Weyl-frame CFT on open solid torus, treating AdS as kinematic geometry recovered only in singular limits, with two-point functions defining entanglement entropy without replicas.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.20415","ref_index":2,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"The dual Ginzburg-Landau theory for a holographic superfluid/superconductor: Critical dynamics","primary_cat":"hep-th","submitted_at":"2026-05-19T19:11:16+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Identifies the dual model F equations for a 5D holographic superconductor/superfluid in the probe limit, obtaining numerical coefficients exactly.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.20321","ref_index":37,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Poles-zeros duality in semi-holographic Mott insulators","primary_cat":"hep-th","submitted_at":"2026-05-19T18:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"A semi-holographic model couples a fermion to a holographic composite sector, yielding poles-zeros duality in the Green's function that distinguishes metallic and Mott-insulating phases through choice of quantization.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.19687","ref_index":13,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Compact objects in AdS spacetime with exponential, quadratic and power-law bosonic mass profiles","primary_cat":"gr-qc","submitted_at":"2026-05-19T11:18:36+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Bosonic compact objects in AdS with three radial mass profiles satisfy Buchdahl compactness limit, observational mass bounds, and null/strong energy conditions, indicating stable non-collapsing models.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.18978","ref_index":3,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"After the Fluid: Subexponential Decay in AdS$_4$","primary_cat":"hep-th","submitted_at":"2026-05-18T18:01:08+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Real-analytic perturbations of AdS4 black branes exhibit stretched-exponential decay exp(-c t^{5/6}) controlled by the large-k tail of the quasinormal mode spectrum.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.17438","ref_index":10,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Holographic entanglement entropy in the QCD phase diagram under external magnetic field","primary_cat":"hep-th","submitted_at":"2026-05-17T13:20:12+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Holographic entanglement entropy exhibits a swallow-tail structure indicating connected-to-disconnected transitions for perpendicular magnetic fields in the QCD phase diagram while remaining monotonic for parallel fields, consistent with black hole thermodynamics.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.17209","ref_index":11,"ref_count":1,"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":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":"2605.16931","ref_index":4,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Nonlinear response of the chiral magnetic effect in the D3/D7 holographic model","primary_cat":"hep-th","submitted_at":"2026-05-16T10:56:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Near the insulating-CME phase boundary in the D3/D7 model, the chiral magnetic current shows multi-valued dependence on magnetic field strength, while axial chemical potential and magnetic field cooperatively stabilize the insulating phase.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.16641","ref_index":4,"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":"[2] O. Aharony, S. S. Gubser, J. M. Maldacena, H. Ooguri, and Y. Oz, \"Large N field theories, string theory and gravity,\" Phys. Rept. 323 (2000) 183-386, arXiv:hep-th/9905111. 75 [3] S. S. Gubser, I. R. Klebanov, and A. M. Polyakov, \"Gauge theory correlators from noncritical string theory,\" Phys. Lett. B 428 (1998) 105-114, arXiv:hep-th/9802109. [4] E. Witten, \"Anti de Sitter space and holography,\" Adv. Theor. Math. Phys. 2 (1998) 253-291, arXiv:hep-th/9802150. [5] O. Aharony, O. Bergman, D. L. Jafferis, and J. Maldacena, \"N=6 superconformal Chern-Simons-matter theories, M2-branes and their gravity duals,\" JHEP 10 (2008) 091, arXiv:0806.1218 [hep-th] . [6] T. Banks, M. R. Douglas, G. T. Horowitz, and E."},{"citing_arxiv_id":"2605.16536","ref_index":2,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Quantum-statistical constraints on Kerr-anti-de Sitter thermodynamics","primary_cat":"gr-qc","submitted_at":"2026-05-15T18:32:30+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Quantum-statistical constraints restrict the infinite family of KadS thermodynamic descriptions to a subclass that reduces to Schwarzschild-AdS and Kerr cases in appropriate limits, with uniqueness for co-rotating and volume-coincident descriptions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.16254","ref_index":71,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Fortuity and Complexity in a Simple Quark Model","primary_cat":"hep-th","submitted_at":"2026-05-15T17:58:25+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":"2605.15776","ref_index":4,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Exact Bulk-Boundary Pairs in AdS/CFT","primary_cat":"hep-th","submitted_at":"2026-05-15T09:33:37+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Exact pairing of CFT two-point functions with interior AdS geodesics on open solid torus via conformal kinematics, without semiclassical approximations.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15478","ref_index":11,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Comments on higher-derivative corrections in the AdS/CFT duality","primary_cat":"hep-th","submitted_at":"2026-05-14T23:36:40+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Prior works on higher-derivative corrections to holographic superconductors may employ an incorrect AdS/CFT dictionary, so that the direction of change in spontaneous condensate depends on the specific model with no universal rule.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.14573","ref_index":3,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Black-hole formation and thermalization in open JT gravity","primary_cat":"hep-th","submitted_at":"2026-05-14T08:43:34+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Numerical simulations show dynamical black hole formation in non-Markovian open JT gravity, corresponding to irreversible thermalization on the boundary.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.13975","ref_index":59,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Protected operators in non-local defect CFTs from AdS","primary_cat":"hep-th","submitted_at":"2026-05-13T18:00:12+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Defect-induced symmetry breaking viewed from the AdS bulk enforces protected displacement and tilt operators in non-local boundary CFTs via Ward identities.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"wherei= 0,1, . . . , d−1 labels the boundary directions andzis the radial coordinate. With these boundary conditions, the bulk gauge field is dual to a dynamical gauge field on the boundary [57, 58]. Ford= 3, one may instead impose electric (Dirichlet) boundary conditions. In that case, the bulk gauge field is dual to a conserved current in the boundary theory [59]. The current operators are then the only operators with scaling dimensions below 3, and they can be used to construct topological surface defects. On such defects, a tilt operator exists, but there is no displacement operator, since the full conformal symmetry is preserved. It is believed that, as the AdS radius is increased from zero to infinity, the Dirichlet theory undergoes a"},{"citing_arxiv_id":"2605.13970","ref_index":6,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"A Tale of Two Hartle-Hawking Wave Functions: Fully Gravitational vs Partially Frozen","primary_cat":"hep-th","submitted_at":"2026-05-13T18:00:07+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"In AdS the fully gravitational Hartle-Hawking wave function acquires a nontrivial one-loop phase while the partially frozen version stays real and positive; a partially frozen de Sitter sphere shows phase cancellation.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.13947","ref_index":65,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Conformal defects and Goldstone bosons in Anti-de Sitter space","primary_cat":"hep-th","submitted_at":"2026-05-13T18:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"Conformal defects in AdS host protected displacement and tilt operators that source bulk Goldstone-like modes with wavelength of order the AdS radius.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.13576","ref_index":36,"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":"Lin,Semifinite von Neumann algebras in gauge theory and gravity,Phys. Rev. D111(2025) 045006 [2407.01695]. [34] J. van der Heijden and E. Verlinde,An operator algebraic approach to black hole information, JHEP02(2025) 207 [2408.00071]. [35] J.M. Maldacena,The Large N limit of superconformal field theories and supergravity,Adv. Theor. Math. Phys.2(1998) 231 [hep-th/9711200]. [36] E. Witten,Anti-de Sitter space and holography,Adv. Theor. Math. Phys.2(1998) 253 [hep-th/9802150]. [37] S.S. Gubser, I.R. Klebanov and A.M. Polyakov,Gauge theory correlators from noncritical string theory,Phys. Lett. B428(1998) 105 [hep-th/9802109]. [38] S. Ryu and T. Takayanagi,Holographic derivation of entanglement entropy from AdS/CFT, Phys. Rev."},{"citing_arxiv_id":"2605.09947","ref_index":36,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"The Free Particle--Oscillator--Inverted Oscillator Triangle: Conformal Bridges, Metaplectic Rotations and $\\mathfrak{osp}(1|2)$ Structure","primary_cat":"hep-th","submitted_at":"2026-05-11T03:51:09+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"The free particle, harmonic oscillator, and inverted oscillator are unified as parabolic, elliptic, and hyperbolic realizations of the same conformal module, with explicit mappings between their states, coherent states, and scattering data via metaplectic rotations and Mellin transforms.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Adv. Math.176(2003) 116-144. [34] J. M. Maldacena,\"The large N limit of superconformal field theories and supergravity,\"Adv. Theor. Math. Phys.2(1998) 231-252; [arXiv:hep-th/9711200]. [35] S. S. Gubser, I. R. Klebanov and A. M. Polyakov,\"Gauge theory correlators from non-critical string theory,\"Phys. Lett. B428(1998) 105-114; [arXiv:hep-th/9802109]. [36] E. Witten,\"Anti de Sitter space and holography,\"Adv. Theor. Math. Phys.2(1998) 253-291; [arXiv:hep-th/9802150]. [37] J.-M. Lévy-Leblond,\"Galilei Group and Nonrelativistic Quantum Mechanics,\"J. Math. Phys.4(1963) 776-788. [38] U. Niederer,\"The maximal kinematical invariance group of the free Schrödinger equation,\" Helv. Phys. Acta45(1972) 802-810."},{"citing_arxiv_id":"2605.05350","ref_index":4,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Challenges to Understanding Celestial Holography from the Bottom Up","primary_cat":"hep-th","submitted_at":"2026-05-06T18:19:53+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Term-by-term celestial transforms of perturbative amplitudes disagree with the full S-matrix transform in the Sinh-Gordon model at leading order.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.05349","ref_index":60,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"All-loop four-quark Bethe-Salpeter kernel","primary_cat":"hep-ph","submitted_at":"2026-05-06T18:19:19+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"The all-loop bare perturbative part of the four-quark Bethe-Salpeter kernel is computed analytically in the large-Nf limit of massless QCD.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"In addition, the pure Yang-Mills theory becomes semi-classical, i.e. the perturbative part of the correlator dominates over the nonperturbative instantonic part suppressed 1 ase −Nc. This approximation has been successfully used throughout the years in e.g. finding the mesonic spectrum of the 't Hooft model [6], establishing the baryon mass scaling by Witten [60], introducing the AdS/CFT correspondence between String and super-Yang-Mills theory [61, 62]. However, each additional loop correction introduces con- tributions from higher-point correlators. For example, a twenty-four-loop gluonic fishnet Feynman diagram for the quark propagator receives a contribution from a four-loop twelve-gluon correlator. Since the all-loop calcu-"},{"citing_arxiv_id":"2605.04621","ref_index":24,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Molien--Weyl Singlet Counting and BFSS$_2$--Factorization in Gaussian Matrix QM","primary_cat":"hep-th","submitted_at":"2026-05-06T08:10:07+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"The very-low-temperature bosonic singlet spectrum in BFSS_{d+1} is controlled by d(d+1)/2 quadratic Gram operators Tr(X_a X_b), with an exact BFSS_3 = (BFSS_2)^3 factorization at (d,N)=(2,2).","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"[22] J. M. Maldacena,The LargeNLimit of Superconformal Field Theories and Supergravity, Adv. Theor. Math. Phys.2, 231 (1998) [Int. J. Theor. Phys.38, 1113 (1999)], arXiv:hep- th/9711200. [23] S. S. Gubser, I. R. Klebanov, and A. M. Polyakov,Gauge Theory Correlators from Non- Critical String Theory, Phys. Lett. B428, 105 (1998), arXiv:hep-th/9802109. [24] E. Witten,Anti-de Sitter Space and Holography, Adv. Theor. Math. Phys.2, 253 (1998), arXiv:hep-th/9802150. [25] K. G. Wilson, \"Confinement of Quarks,\" Phys. Rev. D10, 2445-2459 (1974). [26] Catterall, S. and Wiseman, T., \"Black hole thermodynamics from simulations of lattice Yang-Mills theory,\"Phys. Rev. D78, 041502 (2008). [27] Anagnostopoulos, K."},{"citing_arxiv_id":"2605.04586","ref_index":10,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Bound states and deconfinement from Romans supergravity with magnetic flux","primary_cat":"hep-th","submitted_at":"2026-05-06T07:36:08+00:00","verdict":null,"verdict_confidence":null,"novelty_score":null,"formal_verification":null,"one_line_summary":null,"context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Sonnenschein,Non-critical, near extremal AdS(6) background as a holographic laboratory of four dimensional YM theory,JHEP11(2004) 026 [hep-th/0411009]. [8] R.C. Brower, S.D. Mathur and C.-I. Tan,Glueball spectrum for QCD from AdS supergravity duality,Nucl. Phys. B587 (2000) 249 [hep-th/0003115]. [9] D. Elander, A.F. Faedo, C. Hoyos, D. Mateos and M. Piai,Multiscale confining dynamics from holographic RG flows, JHEP05(2014) 003 [1312.7160]. [10] A.H. Chamseddine and M.S. Volkov,NonAbelian BPS monopoles in N=4 gauged supergravity,Phys. Rev. Lett.79 (1997) 3343 [hep-th/9707176]. [11] I.R. Klebanov and M.J. Strassler,Supergravity and a confining gauge theory: Duality cascades and chi SB resolution of naked singularities,JHEP08(2000) 052 [hep-th/0007191]. [12] J.M. Maldacena and C. Nunez,Towards the large N limit of pure N=1 superYang-Mills,Phys."},{"citing_arxiv_id":"2605.02097","ref_index":45,"ref_count":2,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Separability from Multipartite Measures","primary_cat":"quant-ph","submitted_at":"2026-05-03T23:35:44+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Third-order negativity is a necessary and sufficient criterion for full separability of tripartite pure states and extends to mixed states and qudits.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Tonni,Entanglement negativity in quantum field theory,Phys. Rev. Lett.109(2012) 130502 [1206.3092]. [43] J.M. Maldacena,The LargeNlimit of superconformal field theories and supergravity,Adv. Theor. Math. Phys.2(1998) 231 [hep-th/9711200]. [44] S.S. Gubser, I.R. Klebanov and A.M. Polyakov,Gauge theory correlators from noncritical string theory,Phys. Lett. B428(1998) 105 [hep-th/9802109]. [45] E. Witten,Anti de Sitter space and holography,Adv. Theor. Math. Phys.2 (1998) 253 [hep-th/9802150]. [46] O. Lunin and S.D. Mathur,Correlation functions for M**N / S(N) orbifolds, Commun. Math. Phys.219(2001) 399 [hep-th/0006196]. [47] C.-M. Chang and Y.-H. Lin,Bootstrap, universality and horizons,JHEP10 (2016) 068 [1604.01774]. [48] A. Gadde, V. Krishna and T."},{"citing_arxiv_id":"2605.01573","ref_index":46,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"The atomic nucleus as a bound system of $3A$ quarks","primary_cat":"nucl-th","submitted_at":"2026-05-02T18:55:36+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Nuclei are 3A-quark systems where Fermi gas explains equal u/d quarks in light nuclei, a modified bag model fits heavier ones, and AdS5 duality predicts the lightest glueball's decay and sets the maximum stable nuclear charge at Z=82 for lead.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"particular its mass, depend on its environment [25]. Adquark in a deuteron is not identical to adquark in a lead nucleus10, and the same applies to theuquark. However, all quarks of the same flavor within a given nucleus are identical and indistinguishable. 4 Holographic nuclear physics To enhance the predictive power of the modified bag model, it is useful to employ gauge/gravity duality [45], [46], [47]11. Loosely speaking, this framework posits that much of nuclear and subnuclear physics in Minkowski spaceR1,3 is captured by the physics of black holes (BHs) in five-dimensional anti-de Sitter spaceAdS5 whose boundary isR1,3. 4.1 Refined version of gauge/gravity duality A popular line of research in gauge/gravity duality is to map a BH inAdS5 onto a quark-"},{"citing_arxiv_id":"2604.27068","ref_index":2,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Holographic realization of higher-spin Carrollian free fields","primary_cat":"hep-th","submitted_at":"2026-04-29T18:02:46+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A bulk construction in asymptotically flat higher-spin gravity realizes Carrollian free fields and Miura transformations via generalized boundary conditions and screening charges.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"We dedicate this work to the memory of Robert G. Leigh. We would like to thank Andrea Campoleoni, Adrien Fiorucci, Daniel Grumiller, Chrysoula Markou, Lea Mele and Stefan Prohazka for useful discussions. References [1] J.M. Maldacena,The Large N limit of superconformal field theories and supergravity,Adv. Theor. Math. Phys.2(1998) 231 [hep-th/9711200]. [2] E. Witten,Anti-de Sitter space and holography,Adv. Theor. Math. Phys.2(1998) 253 [hep-th/9802150]. [3] M. Banados, C. Teitelboim and J. Zanelli,The Black hole in three-dimensional space-time, Phys. Rev. Lett.69(1992) 1849 [hep-th/9204099]. [4] M. Gutperle and P. Kraus,Higher Spin Black Holes,JHEP05(2011) 022 [1103.4304]. [5] J.D. Brown and M. Henneaux,Central Charges in the Canonical Realization of Asymptotic"},{"citing_arxiv_id":"2604.26854","ref_index":3,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Deforming ${\\rm AdS}_3\\times S^3\\times T^4$ in Type IIB Supergravity","primary_cat":"hep-th","submitted_at":"2026-04-29T16:20:16+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"New supersymmetric WAdS3 × WS3 × T4 solutions in Type IIB supergravity with independent warp parameters for the AdS and sphere factors, some obtained via two TsT transformations.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"of Research Centres and project ED431F-2023/19), and by the European Union FEDER. References [1] J.M. Maldacena,The Large N limit of superconformal field theories and supergravity,Int. J. Theor. Phys.38(1999) 1113 [hep-th/9711200]. [2] S.S. Gubser, I.R. Klebanov and A.M. Polyakov,Gauge theory correlators from noncritical string theory,Phys. Lett. B428(1998) 105 [hep-th/9802109]. [3] E. Witten,Anti de Sitter space and holography,Adv. Theor. Math. Phys.2(1998) 253 [hep-th/9802150]. [4] A.StromingerandC.Vafa,MicroscopicoriginoftheBekenstein-Hawkingentropy,Phys.Lett. B379(1996) 99 [hep-th/9601029]. [5] A. Strominger,Black hole entropy from near horizon microstates,JHEP02(1998) 009 [hep-th/9712251]. [6] J.D. Brown and M. Henneaux,Central Charges in the Canonical Realization of Asymptotic"},{"citing_arxiv_id":"2604.25035","ref_index":14,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"The Thermodynamics of Cosmological Horizons and Their Holographic Description in de Sitter Space","primary_cat":"hep-th","submitted_at":"2026-04-27T22:35:17+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"A universal first law of thermodynamics for de Sitter cosmological horizons defines entropy in the holographic dual at future infinity as a function of boundary pressure and angular momentum from the Brown-York stress tensor.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"the hologram can be, roughly speaking, taken to live at asymptotic future infinity, denoted byI +, see fig. 1. Some aspects of the holographic dictionary in this case have been worked out, using the analogy with the AdS case as a guide, see [1], also [12]. As is well known, the idea of holography is borne out in a very precise manner in AdS space, [13], [14], see also the review [15], the lecture notes [16-18], the books [19, 20] and the references therein. A key reason to believe that it is more general and applicable also to de Sitter and flat space, stems from the universality of the laws of black hole thermodynamics. These laws suggest quite generally that the number of degrees of freedom in a gravitational"},{"citing_arxiv_id":"2604.24046","ref_index":4,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Low-energy hadronic physics in holographic $\\mathrm{QCD_{3}}$ with anisotropy","primary_cat":"hep-th","submitted_at":"2026-04-27T05:09:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"In an anisotropic holographic model of 3D QCD, hadronic systems become unstable when anisotropy exceeds the confinement energy scale, with dragging terms essential for transport properties.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"theory living on D3-brane in gauge-gravity duality [2, 3], however theN= 4 super Yang-Mills theory is a conformal theory instead of a confined theory. Since our concern of the dual theory is the QCD-like theory as a confined theory, let us demonstrate the construction for a confined theory without supersymmetry in the IIB supergravity with anisotropy. The steps to construct a confined theory in IIB supergravity can also be reviewed in [4, 30]. Specifically, the first step is to compactify the directionyillustrated in Table 1 of the D3- 5 Bubble background t x y (z) u Ω5 Nc D3-branes - - - - ND7 D7-branes - - - - Table 2: The configuration of the D-branes for the bubble solution (2.7). branes on a circleS 1 with the periodδy, so the dual theory becomes effectively three-dimensional"},{"citing_arxiv_id":"2604.21447","ref_index":4,"ref_count":2,"confidence":0.98,"is_internal_anchor":true,"paper_title":"$O(d,d)$ symmetric gravity and finite coupling holography","primary_cat":"hep-th","submitted_at":"2026-04-23T09:06:08+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"In O(d,d) symmetric gravity with curvature corrections, black brane singularities are not resolved but approach with altered Kasner exponents, while a dilaton generates negative cosmological constants at small coupling.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"2(1998) 231 [hep-th/9711200]. - 32 - [2] N. Itzhaki, J.M. Maldacena, J. Sonnenschein and S. Yankielowicz,Supergravity and the large N limit of theories with sixteen supercharges,Phys. Rev. D58(1998) 046004 [hep-th/9802042]. [3] S.S. Gubser, I.R. Klebanov and A.M. Polyakov,Gauge theory correlators from noncritical string theory,Phys. Lett. B428(1998) 105 [hep-th/9802109]. [4] E. Witten,Anti de Sitter space and holography,Adv. Theor. Math. Phys.2(1998) 253 [hep-th/9802150]. [5] E. D'Hoker and D.Z. Freedman,Supersymmetric gauge theories and the AdS / CFT correspondence, inTheoretical Advanced Study Institute in Elementary Particle Physics (TASI 2001): Strings, Branes and EXTRA Dimensions, pp. 3-158, 1, 2002 [hep-th/0201253]."},{"citing_arxiv_id":"2604.21408","ref_index":21,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Holographic complexity of conformal fields in global de Sitter spacetime","primary_cat":"hep-th","submitted_at":"2026-04-23T08:22:52+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Holographic complexity of CFTs in global dS_d is computed via volume and action prescriptions in AdS foliation and brane setups, then compared to results from static and Poincare patches.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Hu,Infrared Behavior of Quantum Fields in Inflationary Cosmology - Issues and Approaches: an overview,1812.11851. [19] M.A. Nielsen, M.R. Dowling, M. Gu and A.C. Doherty,Quantum Computation as Geometry, Science311(2006) 1133 [quant-ph/0603161]. [20] R. Jefferson and R.C. Myers,Circuit complexity in quantum field theory,JHEP10(2017) 107 [1707.08570]. [21] N. Chagnet, S. Chapman, J. de Boer and C. Zukowski,Complexity for Conformal Field Theories in General Dimensions,Phys. Rev. Lett.128(2022) 051601 [2103.06920]. [22] J.M. Maldacena,The LargeNlimit of superconformal field theories and supergravity,Adv. Theor. Math. Phys.2(1998) 231 [hep-th/9711200]. [23] E. Witten,Anti de Sitter space and holography,Adv."},{"citing_arxiv_id":"2604.19418","ref_index":37,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Quantum Spacetime, Quantum Gravity and Gravitized Quantum Theory","primary_cat":"gr-qc","submitted_at":"2026-04-21T12:50:27+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Quantum spacetime with a non-commutative dual explains the fixed Born rule of quantum theory and leads to gravitized quantum mechanics featuring dynamical probabilities and higher-order interference.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Maldacena, \"The Large N limit of superconformal field theories and supergravity,\"Int. J. Theor. Phys. 38(1999) 1113-1133,arXiv:hep-th/9711200 [hep-th]. [Adv. Theor. Math. Phys.2,231(1998)]. [36] S. S. Gubser, I. R. Klebanov, and A. M. Polyakov, \"Gauge theory correlators from noncritical string theory,\" Phys. Lett.B428(1998) 105-114,arXiv:hep-th/9802109 [hep-th]. [37] E. Witten, \"Anti-de Sitter space and holography,\"Adv. Theor. Math. Phys.2(1998) 253-291, arXiv:hep-th/9802150 [hep-th]. [38] L. Freidel, J. Kowalski-Glikman, R. G. Leigh, and D. Minic, \"On the Inevitable Lightness of Vacuum,\" arXiv:2303.17495 [hep-th]. [39] L. Freidel, R. G. Leigh, and D. Minic, \"Modular spacetime,\"Int. J. Mod. Phys.D24no. 12, (2015) 1544028."},{"citing_arxiv_id":"2604.18702","ref_index":9,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Confinement in a finite duality cascade","primary_cat":"hep-th","submitted_at":"2026-04-20T18:02:02+00:00","verdict":null,"verdict_confidence":null,"novelty_score":null,"formal_verification":null,"one_line_summary":null,"context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"5148 [hep-th]. 3, 17 [7] N. Seiberg, \"The Power of holomorphy: Exact results in 4-D SUSY field theories,\" in Particles, Strings, and Cosmology (PASCOS 94), pp. 0357-369. 5, 1994. arXiv:hep-th/9408013. 3 [8] J. M. Maldacena, \"The LargeNlimit of superconformal field theories and supergravity,\" Adv. Theor. Math. Phys.2(1998) 231-252,arXiv:hep-th/9711200. 3 [9] E. Witten, \"Anti de Sitter space and holography,\"Adv. Theor. Math. Phys.2(1998) 253-291,arXiv:hep-th/9802150. 3 [10] S. S. Gubser, I. R. Klebanov, and A. M. Polyakov, \"Gauge theory correlators from noncritical string theory,\"Phys. Lett. B428(1998) 105-114,arXiv:hep-th/9802109. 3 [11] O. Aharony, S. S. Gubser, J. M. Maldacena, H. Ooguri, and Y. Oz, \"Large N field"},{"citing_arxiv_id":"2604.18488","ref_index":3,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Branes","primary_cat":"hep-th","submitted_at":"2026-04-20T16:40:09+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":0.0,"formal_verification":"none","one_line_summary":"A review of branes in string theory covering their multiple descriptions and interaction phenomena.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"branes [1]. While the fundamental string usually provides perturbative degrees of freedom en- 2 coding dynamics of the theory, branes generate and support a background in a non-perturbative fashion. One of the well known examples of such applications of Dp-branes is the AdS/CFT holography first suggested in [2] and then developed in more details in [3,4]. Given the amazing power of holography for investigation of the strong coupling dynamics of quantum field theo- ries, huge amount of various reviews and books is available (we refer the reader to [5-7]). In the most well understood example of the AdS5×S5 AdS/CFT correspondence one considers dynamics of the system of a stack ofND3-branes with open string attached to it and closed"},{"citing_arxiv_id":"2604.15790","ref_index":40,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Holographic Stirling engines and the route to Carnot efficiency","primary_cat":"hep-th","submitted_at":"2026-04-17T07:52:18+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Stirling efficiency reaches Carnot when fixed-volume heat capacity is volume-independent, true for classical gases but not quantum or CFTs; holographic CFTs approach Carnot at large potentials with faster convergence under regeneration.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Phys. D34 (2025), no. 09 2542001 [2508.01830]. [38] J. M. Maldacena,The Large N limit of superconformal field theories and supergravity,Adv. Theor. Math. Phys.2(1998) 231-252 [hep-th/9711200]. [39] S. S. Gubser, I. R. Klebanov and A. M. Polyakov,Gauge theory correlators from noncritical string theory,Phys. Lett. B428(1998) 105-114 [hep-th/9802109]. [40] E. Witten,Anti-de Sitter space and holography,Adv. Theor. Math. Phys.2(1998) 253-291 [hep-th/9802150]. [41] R. Mancilla,Generalized Euler Equation from Effective Action: Implications for the Smarr Formula in AdS Black Holes,2410.06605. [42] S. Borsboom and M. R. Visser,Holographic pressure and volume for black holes, 2602.05130. [43] N. Lilani and M."},{"citing_arxiv_id":"2604.14741","ref_index":11,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"The OPE Approach to Renormalization: Operator Mixing","primary_cat":"hep-th","submitted_at":"2026-04-16T07:53:59+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"OPE-based recursive renormalization for mixed composite operators gives five-loop anomalous dimensions in phi^4 and two-loop in phi^3 models.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Theor. Math. Phys.4(2000) 1149 [hep-th/9912007]. [9] O. Antipin, J. Bersini, F. Sannino, Z.-W. Wang and C. Zhang,Untangling scaling dimensions of fixed charge operators in Higgs theories,Phys. Rev. D103(2021) 125024 [2102.04390]. [10] B. Bajc and A.R. Lugo,Holographic thermal propagator for arbitrary scale dimensions, JHEP05(2023) 103 [2212.13639]. [11] E. Witten,Anti de Sitter space and holography,Adv. Theor. Math. Phys.2(1998) 253 [hep-th/9802150]. - 29 - [12] S.S. Gubser, I.R. Klebanov and A.M. Polyakov,Gauge theory correlators from noncritical string theory,Phys. Lett. B428(1998) 105 [hep-th/9802109]. [13] J.M. Maldacena,The LargeNlimit of superconformal field theories and supergravity,Adv."},{"citing_arxiv_id":"2604.14638","ref_index":1,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"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":"−18E 1(k)E2(k2)E2(k4) + 18E2(k3)E2(k4) + 2E1(k)E1(k2)E3(k4) −12E 1(k2)E3(k5) + 2E1(k)E3(k6) \u0011 m2 + \u0010 81E1(k)5 −474E 1(k)3E1(k2) + 564E1(k)E1(k2)2 −54E 1(k)3E2(k2) + 136E1(k)E1(k2)E2(k2) + 9E1(k)E2(k2)2 + 82E1(k)2E2(k3)−126E 1(k2)E2(k3)−18E 2(k2)E2(k3) −82E 1(k)E2(k4)−2E 1(k)E3(k4) + 6E3(k5) \u0011 m4 + \u0010 42E1(k)3 −80E 1(k)E1(k2)−14E 1(k)E2(k2) + 18E2(k3) \u0011 m6 + 5E1(k)m8 \u0015 . (C.4) References [1] E. Witten,Anti de Sitter space and holography,Adv. Theor. Math. Phys.2(1998) 253 [hep-th/9802150]. [2] S.S. Gubser, I.R. Klebanov and A.M. Polyakov,Gauge theory correlators from noncritical string theory,Phys. Lett. B428(1998) 105 [hep-th/9802109]. - 41 - [3] J.M. Maldacena,The LargeNlimit of superconformal field theories and supergravity,Adv. Theor."},{"citing_arxiv_id":"2604.14492","ref_index":4,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Spinning States and Unitarity in 3D Gravity","primary_cat":"hep-th","submitted_at":"2026-04-16T00:02:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Spinning states scaled with central charge cancel negative densities in 3D gravity, reinterpreted as bulk defects or overspinning BTZ quotients of AdS3 that preserve the gap but exhibit causal pathologies.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"69(1992) 1849-1851, [hep-th/9204099]. [2] M. Banados, M. Henneaux, C. Teitelboim, and J. Zanelli,Geometry of the (2+1) black hole, Phys. Rev. D48(1993) 1506-1525, [gr-qc/9302012]. [Erratum: Phys.Rev.D 88, 069902 (2013)]. - 32 - [3] J. M. Maldacena,The LargeNlimit of superconformal field theories and supergravity,Adv. Theor. Math. Phys.2(1998) 231-252, [hep-th/9711200]. [4] E. Witten,Anti de Sitter space and holography,Adv. Theor. Math. Phys.2(1998) 253-291, [hep-th/9802150]. [5] S. S. Gubser, I. R. Klebanov, and A. M. Polyakov,Gauge theory correlators from noncritical string theory,Phys. Lett. B428(1998) 105-114, [hep-th/9802109]. [6] J. D. Brown and M. Henneaux,Central Charges in the Canonical Realization of Asymptotic"},{"citing_arxiv_id":"2604.14387","ref_index":2,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Emergent States and Algebras from the Double-Scaling limit of Pure States in SYK","primary_cat":"hep-th","submitted_at":"2026-04-15T20:01:32+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"In double-scaled SYK, state-adapted dressed chord operators change the emergent algebra from Type II1 to Type I∞ and restore purity of KM states, unlike generic operators.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"=ψ(n+β+ 1)− 1 β .(D.15) Substituting (D.15) into (D.14), and then settingβ= 2k n =−2n−2ν−1, we arrive at the expectation value of ˆlin thenth bound state: ⟨ˆl⟩n =ψ(−2n−2ν) +ψ(−2n−2ν−1)−ψ(−n−2ν).(D.16) - 81 - References [1] J. M. Maldacena,The Large N limit of superconformal field theories and supergravity, Adv. Theor. Math. Phys.2(1998) 231 [hep-th/9711200]. [2] E. Witten,Anti-de Sitter space and holography,Adv. Theor. Math. Phys.2(1998) 253 [hep-th/9802150]. [3] S. Gubser, I. Klebanov and A. Polyakov,Gauge theory correlators from non-critical string theory,Physics Letters B428(1998) 105-114. [4] S. Antonini, M. Sasieta and B. Swingle,Cosmology from random entanglement,JHEP 11(2023) 188 [2307.14416]. [5] S."},{"citing_arxiv_id":"2604.14335","ref_index":10,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Hofstadter's Butterfly in AdS$_3$ Black Holes","primary_cat":"hep-th","submitted_at":"2026-04-15T18:40:36+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"A single-band lattice model on the BTZ cylinder produces a curvature-dependent Harper equation whose spectra show sharpened butterfly fragmentation at weak curvature and suppressed magnetic response near larger horizons.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.14282","ref_index":52,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Probing Neutrino Compositeness with Invisible and Displaced Signals","primary_cat":"hep-ph","submitted_at":"2026-04-15T18:00:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Neutrinos disintegrate into dark jets in a composite sterile sector, producing enhanced neutral-to-charged current ratios and displaced vertices that probe compositeness scales at facilities like DUNE and FCC-ee.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Beam dump experimentsA single displaced vertex accompanied by a dilepton pair constitutes a generic and essentially background-free signature, yielding a sizable event rate in the kinematic regime relevant for proton beam-dump experiments. This signature was, in fact, the primary target of the CHARM and CHARM II searches for heavy neutral leptons (HNLs) [52, 53]. The corresponding signal yield can be expressed as N1DV(2ℓ) = X M Z dpdΩ dp2 D ΦM(p,Ω) dBR(M→ O N + X) dp2 D P(≥1decay,2ℓ),(2.36) whereΦ M(p,Ω) = d 2NM /dΩdpdenotes the flux of mesonsMwith momentump, which dominate HNL production [46]. The parametrization of this flux is detailed in Section A.3. The differential branching ratio with respect to the DS jet invariant mass is convoluted"},{"citing_arxiv_id":"2604.14046","ref_index":30,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Universality of merons in non-Abelian gauge theories","primary_cat":"hep-th","submitted_at":"2026-04-15T16:23:52+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Merons are universal in many non-Abelian gauge theories and source regular black holes and Euclidean wormholes via a non-Abelian Ayón-Beato-García generalization.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"B. Giddings and A. Strominger, Nucl. Phys. B306, 890 (1988). [26] S. R. Coleman and K.-M. Lee, Nucl. Phys. B329, 387 (1990). [27] S. B. Giddings and A. Strominger, Phys. Lett. B230, 46 (1989). [28] J. M. Maldacena, Adv. Theor. Math. Phys.2, 231 (1998), arXiv:hep-th/9711200. [29] E. Witten, Adv. Theor. Math. Phys.2, 253 (1998), arXiv:hep-th/9802150. [30] S. S. Gubser, I. R. Klebanov, and A. M. Polyakov, Phys. Lett. B428, 105 (1998), arXiv:hep-th/9802109. [31] J. M. Maldacena and L. Maoz, JHEP02, 053 (2004), arXiv:hep-th/0401024. [32] D. Stanford, (2020), arXiv:2008.08570 [hep-th]. [33] T. Hertog, M. Trigiante, and T. Van Riet, JHEP06, 067 (2017), arXiv:1702.04622 [hep-th]. [34] A. Anabal' on and J."}],"limit":50,"offset":0}