{"total":3,"items":[{"citing_arxiv_id":"2607.01334","ref_index":73,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Decoupling band topology from criticality in bosonic systems","primary_cat":"quant-ph","submitted_at":"2026-07-01T18:00:08+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"In a two-parameter family of quadratic bosonic Hamiltonians from a modified bosonic SSH model, topological phase transitions occur along lines of Krein collisions and topological classification holds in both stable and unstable regimes via symplectic Berry phase and index theory.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.10418","ref_index":14,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Higher-winding phases in one-dimensional non-Hermitian topological superconductors","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-06-09T04:49:28+00:00","verdict":"CONDITIONAL","verdict_confidence":"HIGH","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Higher-winding phases with multiple Majorana pairs per end in 1D non-Hermitian topological superconductors are mapped with the Schur-Cohn zero-counting method and confirmed in open-boundary spectra.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.08650","ref_index":31,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Decoding coherent errors in toric codes on honeycomb and square lattices: duality to Majorana monitored dynamics and symmetry classes","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-04-09T18:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"Toric code decodability under coherent X/Z errors is dual to Majorana monitored dynamics whose symmetry class (D or DIII) dictates whether the generic transition is a measurement-induced entanglement transition or a topological transition between area-law phases.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Statistical Model, Majorana Monitored Circuit, and Symmetry Class The syndrome distribution ˜PX({sp}) in|E X ⟩can be written in terms of the partition function ˜ZX({sp}) of a classical disordered statistical model on the square lattice with classical Ising spinsτ v =±1 living on the vertices (see the right panel of Fig. 6): ˜PX({sp}) =| ˜ZX,{sp}|2,(31) where the partition function ˜ZX,{sp} is given by ˜ZX,{sp} =N X {τv=±1} exp  − X ⟨v,v ′⟩ Jv,v ′ηv,v ′τvτv′  .(32) Here,J v,v ′ is a complex nearest-neighbor Ising coupling satisfyinge 2Jv,v′ = i tanθ l for every pair of neighboring sitesvandv ′ connected by the linkl=⟨v, v ′⟩. The variableη v,v ′ =±1 is a random-bond disorder on the square lattice related to the syndromes via Q"}],"limit":50,"offset":0}