{"total":17,"items":[{"citing_arxiv_id":"2607.08070","ref_index":15,"ref_count":1,"confidence":0.55,"is_internal_anchor":false,"paper_title":"(2,m)-threshold quantum data hiding","primary_cat":"quant-ph","submitted_at":"2026-07-09T02:58:24+00:00","verdict":"ACCEPT","verdict_confidence":"HIGH","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A (2,m)-threshold quantum data-hiding scheme is constructed where any pair of m parties can perfectly recover a hidden bit via joint measurement, while LOCC by all parties reveals arbitrarily little information.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.31726","ref_index":64,"ref_count":1,"confidence":0.55,"is_internal_anchor":false,"paper_title":"Entangled photons from para-positronium decay: Do coincidences from scattered photons imply a Bell 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ones, and gives a bound for genuine tripartite entanglement concurrence.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.08189","ref_index":22,"ref_count":1,"confidence":0.55,"is_internal_anchor":false,"paper_title":"Every Rank-Two Entangled State is Projectively Steerable","primary_cat":"quant-ph","submitted_at":"2026-06-06T14:20:05+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"Every rank-two bipartite entangled state is projectively steerable in at least one direction, and two-way steerable when local dimensions match.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.18605","ref_index":13,"ref_count":2,"confidence":0.55,"is_internal_anchor":false,"paper_title":"Non-Gaussian Entanglement Hierarchy Based on the Schmidt Number","primary_cat":"quant-ph","submitted_at":"2026-05-18T16:15:17+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Defines witness E_NG whose ceiling lower-bounds the Gaussian-irreducible Schmidt number, creating an operational hierarchy for non-Gaussian entanglement in continuous-variable systems.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.14644","ref_index":4,"ref_count":1,"confidence":0.55,"is_internal_anchor":false,"paper_title":"Generating Non-Decomposable Maps with Differentiable Semidefinite Programming","primary_cat":"quant-ph","submitted_at":"2026-05-14T10:01:29+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"A differentiable SDP method generates positive non-decomposable maps, identifies parametrized families, and explores open problems like the PPT square conjecture.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.05633","ref_index":57,"ref_count":1,"confidence":0.55,"is_internal_anchor":false,"paper_title":"Eigenstate-Selective Entangled Two-Photon Absorption in Monolayer WSe$_2$","primary_cat":"quant-ph","submitted_at":"2026-05-07T03:37:13+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Bell-state phase of entangled photons partitions biexciton excitations between bright and exchange-dark eigenstates in WSe2 via independent valley pathways, with >0.97 visibility at 4 K.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.03022","ref_index":60,"ref_count":1,"confidence":0.55,"is_internal_anchor":false,"paper_title":"General method for obtaining the energy minimum of spin Hamiltonians for separable states","primary_cat":"quant-ph","submitted_at":"2026-05-04T18:00:16+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A method is given to compute the minimum energy of certain spin Hamiltonians over separable states, expressed via quantum Fisher information for Ising models and fidelity for Heisenberg chains.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.25640","ref_index":34,"ref_count":1,"confidence":0.55,"is_internal_anchor":false,"paper_title":"Continuous Reset-Induced Phase Transition in Measurement-Free Random Quantum Circuits","primary_cat":"quant-ph","submitted_at":"2026-04-28T13:40:52+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Reset-induced entanglement phase transitions in measurement-free random quantum circuits are continuous for d=2 with second-order characteristics, unlike large-d classical expectations.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.19333","ref_index":13,"ref_count":1,"confidence":0.55,"is_internal_anchor":false,"paper_title":"Generating pairwise entanglement in periodically driven quantum spin chains with stochastic resetting","primary_cat":"quant-ph","submitted_at":"2026-04-21T11:05:06+00:00","verdict":"CONDITIONAL","verdict_confidence":"MODERATE","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Stochastic resetting produces finite pairwise concurrence in the steady state of periodically driven XY and Rydberg spin chains, with a critical rate below which it vanishes and an optimal rate at which it peaks.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.12576","ref_index":42,"ref_count":1,"confidence":0.55,"is_internal_anchor":false,"paper_title":"Detecting entanglement from few partial transpose moments and their decay via weight enumerators","primary_cat":"quant-ph","submitted_at":"2026-04-14T10:56:59+00:00","verdict":"ACCEPT","verdict_confidence":"HIGH","novelty_score":6.5,"formal_verification":"none","one_line_summary":"Any three PT moments of orders k<l<m certify NPT entanglement if p_l > p_k^x p_m^{1-x}, and Stieltjes-m equals PPT when ρ^Γ has at most (m+1)/2 distinct eigenvalues.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2601.03694","ref_index":59,"ref_count":1,"confidence":0.55,"is_internal_anchor":false,"paper_title":"Interference-Induced Suppression of Doublon Transport and Prethermalization in the Extended Bose-Hubbard 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mixed-state magic, proves multi-qubit distillation is strictly stronger than single-qubit schemes, and identifies a purity bound plus undetectable unfaithful magic states.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2512.07822","ref_index":17,"ref_count":1,"confidence":0.55,"is_internal_anchor":false,"paper_title":"Comparing quantum channels using Hermitian-preserving trace-preserving linear maps: A physically meaningful approach","primary_cat":"quant-ph","submitted_at":"2025-12-08T18:54:22+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"A quantum channel A is physically harder to implement than channel B if A's output statistics allow unique identification of the input state from B's output via some measurement, which is equivalent to obtaining A from B by post-composition with an HPTP 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Systems","primary_cat":"quant-ph","submitted_at":"2025-10-06T08:52:18+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"A multipartite pure state is 2-producible if and only if all generalized entanglement of purification gaps vanish.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2510.02256","ref_index":29,"ref_count":1,"confidence":0.55,"is_internal_anchor":false,"paper_title":"Fate of entanglement in open quantum spin liquid: Time evolution of its genuine multipartite negativity upon sudden coupling to a dissipative bosonic environment","primary_cat":"cond-mat.str-el","submitted_at":"2025-10-02T17:39:53+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Time evolution of genuine multipartite negativity in the open Kitaev quantum spin liquid shows persistence in loopy subregions in Markovian regime and at higher temperatures in non-Markovian regime.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}