{"total":16,"items":[{"citing_arxiv_id":"2607.08481","ref_index":39,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Gram--Wishart--Stiefel formulation of the $N=2$, large--$d$ gauge theory in 1D","primary_cat":"hep-th","submitted_at":"2026-07-09T13:40:18+00:00","verdict":"CONDITIONAL","verdict_confidence":"MODERATE","novelty_score":5.5,"formal_verification":"none","one_line_summary":"Gram/Wishart/Stiefel reformulation of N=2 large-d BFSS/BMN endpoints absorbs -A into a shifted mass and recovers the universal continuum -2d DΛ-channel after non-polynomial transverse completion.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.21662","ref_index":37,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"On the Universality of Probe Complexity in $\\mathcal{N}=4$ SYM","primary_cat":"hep-th","submitted_at":"2026-06-19T18:08:51+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Protected and few-body sectors in N=4 SYM exhibit integrable Krylov dynamics with a_n=2Mg and b_n→Mg, insufficient for testing gravitational universality of complexity growth; a finite-density program is proposed to test dependence only on coarse thermodynamic data.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.20353","ref_index":5,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Fortuity beyond counting: an explicit construction","primary_cat":"hep-th","submitted_at":"2026-06-18T15:19:02+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Explicit construction of BPS states in (h,j)=(1,0) sector of D1D5 CFT shows non-vanishing three-point coupling between monotone and fortuitous states, indicating the sectors are dynamically connected.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.17758","ref_index":39,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"A Double--Scaling Large--\\(d\\) Saddle of BFSS/BMN Matrix Quantum Mechanics","primary_cat":"hep-th","submitted_at":"2026-06-16T10:24:05+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":"2606.09521","ref_index":98,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Negative heat capacities in spherically symmetric sectors of $d$-matrix quantum mechanics","primary_cat":"hep-th","submitted_at":"2026-06-08T14:10:20+00:00","verdict":"CONDITIONAL","verdict_confidence":"MODERATE","novelty_score":6.0,"formal_verification":"none","one_line_summary":"In SO(d)- and O(d)-invariant sectors of the U(N) d-matrix harmonic oscillator, microcanonical heat capacity is negative at low energy and turns positive at kcrit ~ N^2/4, producing a caloric fold analogous to AdS black holes.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.26055","ref_index":38,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Krylov Complexity for Plane Wave Matrix Model","primary_cat":"hep-th","submitted_at":"2026-05-25T17:15:34+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"In reduced BMN matrix models, Lanczos coefficients scale linearly with the mass parameter, producing quadratic corrections to early-time Krylov complexity growth at the same order for both state and operator versions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.25647","ref_index":39,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Endpoint formulation and Molien--Weyl structure for the \\(N=2\\), large--\\(d\\) BFSS/BMN models","primary_cat":"hep-th","submitted_at":"2026-05-25T09:53:14+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Establishes equivalence between endpoint and Molien-Weyl formulations for large-d BFSS models on the lattice and derives finite continuum D-channel via a toy holonomy potential model.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.16254","ref_index":2,"ref_count":2,"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":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"In a toy qubit model of quarks, baryons are fortuitous with exponential counting and super-exponential complexity while mesons are monotone with polynomial counting and power-law complexity.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.14726","ref_index":9,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Holographic interpolations of codimension-2 defect CFTs","primary_cat":"hep-th","submitted_at":"2026-05-14T11:53:45+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":0.0,"formal_verification":"none","one_line_summary":"Review of holographic interpolations and one-point functions for codimension-2 defect CFTs in weak and strong coupling.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.27087","ref_index":37,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Oscillators from non-semisimple walled Brauer algebras","primary_cat":"hep-th","submitted_at":"2026-04-29T18:30:43+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Dimension corrections in non-semisimple walled Brauer algebras are counted via restricted Bratteli diagrams whose generating functions match the partition function of an infinite tower of simple harmonic oscillators.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.23287","ref_index":16,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Chaos of Berry curvature for BPS microstates","primary_cat":"hep-th","submitted_at":"2026-04-25T13:03:42+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Berry curvature of BPS states is random-matrix-like for supersymmetric black hole microstates but non-random and often zero for horizonless geometries, offering a chaos diagnostic in degenerate sectors.","context_count":1,"top_context_role":"background","top_context_polarity":"support","context_text":"by slowly varying the couplings in time, a state|a⟩ ∈H n(λ(0)) will mix under evolution with all the other states in this degenerate subspace, but not with the states outside it. Schr¨ odinger's equation for such an evolution then implies that the mixing matrixUis a unitary matrix determined by aD×DHermitian matrix-valued connectionAforH n(λ) over the moduli spaceM, known as the Berry connection [16, 17] (or Wilczek-Zee connection in the degenerate case [18]). There is a corresponding curvature for this connection,F=dA−iA∧A, known as the Berry curvature. In quantum mechanics, the curvature can be computed in perturbation theory around any point, and it reads Fµν \u0001 ab = X m̸∈Hn i⟨b|∂ [µH|m⟩ ⟨m|∂ ν]H|a⟩ (En −E m)2 .(1.1) If the evolution is along a loopγ, illustrated in Figure 1, then the mixing matrixUis the"},{"citing_arxiv_id":"2603.28880","ref_index":18,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Holographic two-point functions of heavy operators revisited","primary_cat":"hep-th","submitted_at":"2026-03-30T18:03:39+00:00","verdict":"CONDITIONAL","verdict_confidence":"MODERATE","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Holographic two-point functions of heavy operators are reproduced by adding boundary terms to the D3-brane action and by the Gibbons-Hawking-York term in LLM backgrounds, but only in coordinate dependence and without normalization.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"point function was recovered by evaluating the on-shell action for the AdS-Schwarzschild geometry in [16, 17]. For the two-point functions of half-BPS operators one expects the supergravity background to be also half-BPS, and the most general non-singular background which preserves half of the supersymmetries and hasR×SO(4)×SO(4)symmetry of the two-point function were constructed by Lin, Lunin, and Maldacena in [18] (for brevity, we call them LLM backgrounds in the following). One can verify that the LLM background is, in fact, the geometry created by the insertion of two heavy (∆∼N2) half-BPS operators by performing a probe analysis: one inserts a third light (∆∼1) operator on the boundary and does GKPW analysis in the LLM background to extract the three-point function and"},{"citing_arxiv_id":"2511.18128","ref_index":40,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Supersymmetric AdS Solitons, Coulomb Branch Flows and Twisted Compactifications","primary_cat":"hep-th","submitted_at":"2025-11-22T17:23:37+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Constructs holographic supergravity solutions for supersymmetric RG flows from 4D SCFTs to confining 3D SQFTs, with universal factorization of observables.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2508.20094","ref_index":20,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"(Un)solvable Matrix Models for BPS Correlators","primary_cat":"hep-th","submitted_at":"2025-08-27T17:58:07+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Proposes complex matrix models for BPS correlators in N=4 SYM, relating eigenvalue distributions to LLM droplet shapes and enabling computations of one-point functions and three-point correlators via reductions to known models.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"gauge theory to the eigenvalue dynamics of a single matrix, which is equivalent toNfree fermions 3 in a harmonic trap [19]. The half-BPS state wavefunctions can be associated with Fermi droplet configurations on a 2d plane. This description in terms of droplets precisely matches the boundary conditions for half-BPS solutions of type IIB supergravity [20]. The metric and field profiles of such solutions are uniquely determined from a potential function determined from the density of fermions on the plane. The Fermi sea of the fermions is identified with the regions of the spacetime on the boundary of which the topology change occurs [20] in the dual description. Since this relies on an understanding of the collective eigenvalue variables as opposed to the gauge invariant operators"},{"citing_arxiv_id":"2406.19441","ref_index":79,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Moduli Spaces in CFT: Large Charge Operators","primary_cat":"hep-th","submitted_at":"2024-06-27T18:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"CFTs with broken continuous global symmetry on the moduli space require a tower of charged local operators whose scaling dimensions are asymptotically linear in the charge.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"1906.11515","ref_index":42,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Structure Constants of a Single Trace Operator and Determinant Operators from Hexagon","primary_cat":"hep-th","submitted_at":"2019-06-27T09:31:40+00:00","verdict":"CONDITIONAL","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Conjecture that the three-point structure constant of one single-trace and two determinant operators in N=4 SYM is given by glued hexagon form factors, reducing to partition sums with reflections at weak coupling and matching explicit tree-level computations.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}