{"total":11,"items":[{"citing_arxiv_id":"2607.07786","ref_index":16,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Chiral Tube Algebras I: Topological Defect Lines, Twisted Modules, and Finite Gauging","primary_cat":"hep-th","submitted_at":"2026-07-08T18:00:00+00:00","verdict":"ACCEPT","verdict_confidence":"HIGH","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Chiral tube algebras unify chiral algebras and TDLs by acting on twisted defect spaces via local and non-local currents, with modules isomorphic to twisted modules of the parent algebras.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.32035","ref_index":16,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Exactly solvable non-unitary conformal interfaces in unitary CFTs","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-30T17:58:56+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"An SL(2,C)-parametrized family of exactly solvable non-unitary conformal interfaces is constructed on the lattice in unitary CFTs via analytic continuation, leading to a non-unitary Cardy condition and logarithmic entanglement with generally complex effective central charge.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.30720","ref_index":51,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Complex Conformal Manifolds","primary_cat":"hep-th","submitted_at":"2026-06-29T18:00:01+00:00","verdict":"CONDITIONAL","verdict_confidence":"MODERATE","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Complexified exactly-marginal couplings produce solvable complex CFTs, with the Ising defect verified numerically in non-Hermitian chains.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.24812","ref_index":7,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Radial Mirror Scattering and the QNM Convergence Region","primary_cat":"gr-qc","submitted_at":"2026-06-23T16:59:05+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"A reflection about a distinguished point in the tortoise coordinate maps the Regge-Wheeler problem to a mirror version with the same QNM spectrum and provides an image interpretation of the lightcone distance controlling convergence of Schwarzschild retarded Green functions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.27193","ref_index":105,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Algebras of order parameters in one-dimensional spin systems","primary_cat":"cond-mat.str-el","submitted_at":"2026-05-26T15:45:35+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"String order parameters in 1D gapped phases with invertible or non-invertible symmetries organize into Lagrangian algebras in the Drinfel'd centre via tensor-network module categories.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.20688","ref_index":46,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Fusion of Integrable Defects and the Defect $g$-Function","primary_cat":"hep-th","submitted_at":"2026-05-20T04:34:22+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Derives additivity and fusion rules for defect g-functions in integrable 2D QFT, with effective amplitudes for non-topological cases and lowered entropy contribution in Ising non-topological fusion.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.14580","ref_index":6,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Scattering off Chamblin-Reall Branes","primary_cat":"hep-th","submitted_at":"2026-05-14T08:51:27+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Holographic analysis of scattering off Chamblin-Reall branes shows that for d>1 incident radiation redistributes into reflected, transmitted, and evanescent components, with d=2 yielding diffuse scattering like a translucent window and d=4 requiring IR regulation.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.13961","ref_index":87,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"A Twist on Scattering from Defect Anomalies","primary_cat":"hep-th","submitted_at":"2026-05-13T18:00:02+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Defect 't Hooft anomalies trap charges at symmetry-line junctions and thereby drive categorical scattering into twist operators.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"charged wavepackets according to our arguments. Furthermore, we will see that in the XYZ model we can construct in this manner nontrivial interfaces which are not connected to topological (transmissive) ones by deformations localized on the defect. 7.1 Order/Disorder Interface in Ising A paradigmatic example is provided by the Ising model, whose interfaces have been classified in [87]. We will focus on an interface between the ordered and disordered descriptions of the Ising model [22]. This is also the lattice regularization of the model presented in Section 6. Recall that the Ising Hamiltonian: HIsing =− X j XjXj+1 −h X j Zj ,(7.5) flows to aZ 2 ordered/disordered phase forh >1 andh <1, respectively. In (7.5),XandZdenote respectively the X and Z Pauli matrices acting on the two-dimensional Hilbert space localized at"},{"citing_arxiv_id":"2601.03879","ref_index":3,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Defects in N=1 minimal models and RG flows","primary_cat":"hep-th","submitted_at":"2026-01-07T12:47:19+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Topological defects constrain the allowed RG flows of N=1 superconformal minimal models, first via a bosonic coset description and then for the full superconformal case.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2509.13404","ref_index":15,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Decoding the string in terms of holographic quantum maps","primary_cat":"hep-th","submitted_at":"2025-09-16T18:00:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Stringy modes in 3D gravitational junctions map to factorized H_in to H_out and H_L to H_R quantum maps involving scattering matrices and relative Virasoro automorphisms in the dual CFT.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2308.00747","ref_index":4,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"What's Done Cannot Be Undone: TASI Lectures on Non-Invertible Symmetries","primary_cat":"hep-th","submitted_at":"2023-08-01T18:00:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"A survey of non-invertible symmetries with constructions in the Ising model and applications to neutral pion decay and other systems.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"In this section we discuss the simplest nontrivial example of the non-invertible global symmetry - the Kramers-Wannier duality defect in the 1+1d critical Ising model, which is arguably the simplest quantum system beyond quantum mechanics. There are at least six constructions of the non-invertible symmetry in the Ising model: • Topological defect line in Ising CFT [4, 5, 9, 28]. • From the chiral symmetry of the Majorana CFT via bosonization [154, 30, 66]. • Half gauging and the Kramers-Wannier duality [65]. • Non-invertible lattice operator [63, 155] and the duality defect [156] in the transverse-field Ising lattice model. • Aasen-Fendley-Mong (AFM) construction in the statistical Ising model [25, 26]. • Anyonic chain and its generalization [13, 157-159, 26]."}],"limit":50,"offset":0}