{"paper":{"title":"Chiral Multiplets of Heavy-Light Mesons","arxiv_id":"hep-ph/0305049","primary_cat":"hep-ph","submitted_at":"2003-05-05T19:36:07+00:00","version_compiled":"v2"},"notice":"Every quoted sentence is the authors' text from the arXiv listing abstract. Labels and probabilities are the outputs of classifier-1.13-20260917 on the question bank abstract-p1-20260923, exactly as returned. No sentence in this record was written by a language model.","schema":"pith.compiled-record/v0","status":"compiled","abstract":{"source":"arXiv listing abstract v2","sentences":[{"i":0,"p":0.49,"id":"s0","own":false,"role":"interpretation","text":"The recent discovery of a narrow resonance in D_s+pi^0 by the BABAR collaboration is consistent with the interpretation of a heavy J^P(0+,1+) spin multiplet.","hedge":{"p":1.0,"label":"hedged_possibility"},"own_p":0.08,"main_claim_p":0.46,"quantitative":false,"quantitative_p":0.25,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.07,"background":0.42,"limitation":0.0,"future_work":0.0,"contribution":0.02,"interpretation":0.49}},{"i":1,"p":0.84,"id":"s1","own":true,"role":"interpretation","text":"This system is the parity partner of the groundstate (0-,1-) multiplet, which we argue is required in the implementation of SU(3)_L x SU(3)_R chiral symmetry in heavy-light meson systems.","hedge":{"p":0.69,"label":"asserted"},"own_p":0.52,"main_claim_p":0.26,"quantitative":false,"quantitative_p":0.2,"role_probabilities":{"gap":0.0,"method":0.01,"result":0.0,"background":0.11,"limitation":0.0,"future_work":0.0,"contribution":0.04,"interpretation":0.84}},{"i":2,"p":0.86,"id":"s2","own":true,"role":"result","text":"The (0+,1+)->(0-,1-)+pi transition couplings satisfy a Goldberger-Treiman relation, g_pi = Delta(M)/f_pi, where Delta(M) is the mass gap.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.61,"main_claim_p":0.13,"quantitative":false,"quantitative_p":0.23,"role_probabilities":{"gap":0.0,"method":0.02,"result":0.86,"background":0.02,"limitation":0.0,"future_work":0.0,"contribution":0.04,"interpretation":0.06}},{"i":3,"p":0.63,"id":"s3","own":false,"role":"interpretation","text":"The BABAR resonance fits the 0+ state, with a kinematically blocked principal decay mode to D+K.","hedge":{"p":0.96,"label":"asserted"},"own_p":0.35,"main_claim_p":0.09,"quantitative":false,"quantitative_p":0.33,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.37,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.63}},{"i":4,"p":0.94,"id":"s4","own":true,"role":"result","text":"The allowed D_s+pi, D_s+2pi and electromagnetic transitions are computed from the full chiral theory and found to be suppressed, consistent with the narrowness of the state.","hedge":{"p":0.99,"label":"asserted"},"own_p":0.92,"main_claim_p":0.14,"quantitative":false,"quantitative_p":0.29,"role_probabilities":{"gap":0.0,"method":0.01,"result":0.94,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.01,"interpretation":0.04}},{"i":5,"p":0.82,"id":"s5","own":true,"role":"interpretation","text":"This state establishes the chiral mass difference for all such heavy-quark chiral multiplets, and precise predictions exist for the analogous B_s and strange doubly-heavy baryon states.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.7,"main_claim_p":0.44,"quantitative":false,"quantitative_p":0.06,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.13,"background":0.0,"limitation":0.0,"future_work":0.03,"contribution":0.02,"interpretation":0.82}}]},"compiled":{"main_claim":{"p":0.62,"text":"The recent discovery of a narrow resonance in D_s+pi^0 by the BABAR collaboration is consistent with the interpretation of a heavy J^P(0+,1+) spin multiplet.","location":"abstract s0","hedge_strength":{"p":1.0,"label":"hedged possibility"}},"provenance":{"route":{"via":"OpenRouter","model":"classifier-1.13","endpoint":"https://openrouter.ai/api/v1/systemone","provider":"TypeSafe"},"packing":"one request per paper","requests":1,"input_tokens":5090,"cost_usd_reported":0.000214},"compiled_at":"2026-09-23","bank_version":"abstract-p1-20260923","model_version":"classifier-1.13-20260917","abstract_states":{"claims_first":0.04,"states_limitation":0.15,"human_participants":0.01,"controlled_comparison":0.03,"randomized_assignment":0.01,"states_quantitative_result":0.3,"compares_with_prior_results":0.6,"mentions_code_or_data_availability":0.02},"evidential_basis":{"p":0.55,"value":"argument","probabilities":{"argument":0.55,"literature":0.04,"proof_or_derivation":0.04,"analysis_of_existing_data":0.33,"observation_or_experiment":0.01,"simulation_or_computation":0.03}},"contribution_type":{"p":0.95,"value":"theoretical result","probabilities":{"review":0.0,"method_or_tool":0.0,"empirical_study":0.0,"simulation_study":0.0,"theoretical_result":0.95,"dataset_or_benchmark":0.0,"position_or_commentary":0.05}},"contribution_statement":{"p":0.79,"text":"The allowed D_s+pi, D_s+2pi and electromagnetic transitions are computed from the full chiral theory and found to be suppressed, consistent with the narrowness of the state.","location":"abstract s4"}},"coverage":{"tier":"abstract","levels_run":["P abstract"],"not_examined":["full text","figures and tables","references and citing sentences","relations to other papers"],"sources_read":["arXiv listing abstract v2"],"levels_not_run":["S sections","T body sentences","C citations","R cross-paper relations"],"sentences_examined":6,"sentences_in_abstract":6},"measured_accuracy":{"url":"https://pith.science/accuracy","measured_on":"2026-10-02","method":"two independent model families labelled a fresh random sample blind; the figure is how often the published label matches their consensus","sentence_role_agreement":0.92,"main_claim_agreement":0.908,"typed_citation_agreement":0.933,"typed_citation_agreement_95_interval":[0.917,0.945],"review_comments_accurate":0.758,"review_comments_accurate_95_interval":[0.684,0.82],"review_caught_admitted_error_found_or_related":0.448}}