{"total":6,"items":[{"citing_arxiv_id":"2606.08917","ref_index":18,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Electromagnetism from two matter spaces: mutual helicity and the nondegenerate completion","primary_cat":"gr-qc","submitted_at":"2026-06-08T01:47:42+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Generic Maxwell fields are obtained as the sum of two pull-backs from independent matter spaces, recovering the F wedge F invariant as mutual helicity between the two sectors.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.03619","ref_index":3,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"The Polymorphic Chiral Anomaly","primary_cat":"hep-ph","submitted_at":"2026-06-02T13:20:15+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Derives a generic chiral anomaly formula incorporating multiple Feynman diagrams, from which abelian, singlet, consistent, and covariant forms follow, with topological discussion and FeynCalc code.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.28035","ref_index":7,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Topological Susceptibility and QCD at Finite Theta Angle","primary_cat":"hep-lat","submitted_at":"2026-04-30T15:47:45+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":1.0,"formal_verification":"none","one_line_summary":"A pedagogical review summarizing analytic predictions and recent lattice results for theta-dependence and topological susceptibility in QCD.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Actor, Classical solutions ofSU(2)yang-mills theories, Rev. Mod. Phys. 51 (1979) 461-525.doi:10.1103/RevModPhys.51.461. [5] C. Vafa, E. Witten, Parity Conservation in QCD, Phys. Rev. Lett. 53 (1984) 535.doi:10.1103/PhysRevLett.53.535. [6] S. L. Adler, Axial vector vertex in spinor electrodynamics, Phys. Rev. 177 (1969) 2426-2438.doi:10.1103/PhysRev.177.2426. [7] J. S. Bell, R. Jackiw, A PCAC puzzle:π 0 →γγin theσmodel, Nuovo Cim. A 60 (1969) 47-61.doi:10.1007/BF02823296. [8] G. 't Hooft, Symmetry Breaking Through Bell-Jackiw Anomalies, Phys. Rev. Lett. 37 (1976) 8-11.doi:10.1103/PhysRevLett.37.8. [9] S. Weinberg, The U(1) Problem, Phys. Rev. D 11 (1975) 3583-3593.doi:10.1103/PhysRevD.11.3583. [10] G. 't Hooft, A Planar Diagram Theory for Strong Interactions, Nucl."},{"citing_arxiv_id":"2512.18382","ref_index":298,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Lepton anomalous magnetic moments: Theory","primary_cat":"hep-ph","submitted_at":"2025-12-20T14:46:51+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"The paper provides an overview of theoretical calculations for lepton anomalous magnetic moments arising from quantum corrections in the Standard Model.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.02005","ref_index":32,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Renormalisation","primary_cat":"hep-ph","submitted_at":"2025-11-03T19:19:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":1.0,"formal_verification":"none","one_line_summary":"An introductory review of renormalisation procedures, the renormalisation group, and scale-setting optimisation in gauge theories such as QCD.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"effective field theories (EFT) (e.g. see Ref. [ 30]) or for the operator product expansion (OPE) , where operators with higher dimensions are introduced and mix under renormalisation [ 6]. On the contrary, the Axial-vector-current Ward identity is not preserved perturbatively not even for a chiral Lagrangi an, due to the occurrence of the ABJ-anomaly (Adler, Bell and Jackiw [ 31] [32]) from the triangular diagrams: b c a J A λ JV µ JV ν > > > + b c a J A λ JV µ JV ν > > > Fig. 6 Feynman diagrams responsible for the anomaly of a gauge symm etry current in a chiral gauge theory . The contributions of the two diagrams in Fig. 6, does not cancel and in the Abelian case they result: ∂λJA λ = 1 16π2εαβγδFαβFγδ, (71) with JA µ = ¯ψγµγ5ψand JV"},{"citing_arxiv_id":"2412.03588","ref_index":49,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Spectral Networks: Bridging higher-rank Teichm\\\"uller theory and BPS states","primary_cat":"math-ph","submitted_at":"2024-11-27T10:11:29+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":0.0,"formal_verification":"none","one_line_summary":"A comprehensive introduction to spectral networks that develops higher-rank Teichmüller theory in parallel with class S gauge theory and BPS spectra.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"with a geometry. For surfaces of genus at least 2, this leads to hyperbolic geometry. Themodelspaceisthehyperbolicplane.Wegiveabriefintroductiontothebeautiful worldofhyperbolicgeometryindimension2startingfromthehyperbolicplaneand its isometries and then discussing hyperbolic surfaces. References for an extended treatment include, for example, [344] or [49], [257], [308]. 4.1 The hyperbolic plane In dimension 2, there are three types of geometry: Euclidean geometry which is taught at school, spherical and hyperbolic geometry. They are distinguished by the curvatureoftheunderlyingspace:zerofortheEuclideanplane,1fortheunitsphere and −1 for the hyperbolic plane. To be more precise, the hyperbolic plane H is the unique complete, sim-"}],"limit":50,"offset":0}