{"paper":{"title":"Model-independent predictions for decays of double-heavy hadrons into pairs of heavy hadrons","arxiv_id":"2408.05150","primary_cat":"hep-ph","submitted_at":"2024-08-09T16:14:02+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-1.13.0 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":0.87,"id":"s0","own":false,"role":"background","text":"Double-heavy hadrons can decay into pairs of heavy hadrons through transitions from confining Born-Oppenheimer potentials to heavy-hadron-pair potentials with the same Born-Oppenheimer quantum numbers.","hedge":{"p":0.63,"label":"asserted"},"own_p":0.15,"main_claim_p":0.14,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.04,"result":0.01,"background":0.87,"limitation":0.0,"future_work":0.0,"contribution":0.08,"interpretation":0.0}},{"i":1,"p":0.72,"id":"s1","own":false,"role":"background","text":"The states of the double-heavy hadron are constrained by a Born-Oppenheimer exclusion principle from the identical heavy quarks.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.15,"main_claim_p":0.05,"quantitative":false,"quantitative_p":0.08,"role_probabilities":{"gap":0.0,"method":0.17,"result":0.04,"background":0.72,"limitation":0.0,"future_work":0.0,"contribution":0.07,"interpretation":0.0}},{"i":2,"p":0.84,"id":"s2","own":false,"role":"background","text":"The states of a pair of identical heavy hadrons are constrained by exclusion principles from identical particles.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.09,"main_claim_p":0.04,"quantitative":false,"quantitative_p":0.05,"role_probabilities":{"gap":0.0,"method":0.09,"result":0.02,"background":0.84,"limitation":0.0,"future_work":0.0,"contribution":0.05,"interpretation":0.0}},{"i":3,"p":0.57,"id":"s3","own":false,"role":"background","text":"The transitions are also constrained by conservation of angular momentum and parity.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.16,"main_claim_p":0.04,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.34,"result":0.01,"background":0.57,"limitation":0.01,"future_work":0.0,"contribution":0.07,"interpretation":0.0}},{"i":4,"p":0.52,"id":"s4","own":true,"role":"result","text":"From these constraints, we derive model-independent selection rules for decays of double-heavy hadrons into pairs of heavy hadrons.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.95,"main_claim_p":0.78,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.52,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.48,"interpretation":0.0}},{"i":5,"p":0.86,"id":"s5","own":true,"role":"method","text":"The coupling potentials are expressed as sums of products of Born-Oppenheimer transition amplitudes and angular-momentum coefficients.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.81,"main_claim_p":0.06,"quantitative":false,"quantitative_p":0.05,"role_probabilities":{"gap":0.0,"method":0.86,"result":0.03,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.11,"interpretation":0.0}},{"i":6,"p":0.88,"id":"s6","own":true,"role":"result","text":"If there is a single dominant Born-Oppenheimer transition amplitude, it factors out of the coupling potentials between double-heavy hadrons in the same Born-Oppenheimer multiplet and pairs of heavy hadrons in specific heavy-quark-spin-symmetry multiplets and out of the corresponding partial decay rates.","hedge":{"p":0.76,"label":"asserted"},"own_p":0.82,"main_claim_p":0.23,"quantitative":false,"quantitative_p":0.28,"role_probabilities":{"gap":0.0,"method":0.04,"result":0.88,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.04,"interpretation":0.04}},{"i":7,"p":0.98,"id":"s7","own":true,"role":"contribution","text":"As examples, we discuss the Born-Oppenheimer potentials and multiplets for conventional double-heavy baryons and for double-heavy tetraquark mesons.","hedge":{"p":0.84,"label":"asserted"},"own_p":0.84,"main_claim_p":0.04,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.02,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.98,"interpretation":0.0}},{"i":8,"p":0.81,"id":"s8","own":true,"role":"contribution","text":"We also discuss the relative partial decay rates for conventional double-heavy baryons into pairs of heavy hadrons.","hedge":{"p":0.57,"label":"asserted"},"own_p":0.87,"main_claim_p":0.06,"quantitative":false,"quantitative_p":0.19,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.19,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.81,"interpretation":0.0}}]},"compiled":{"main_claim":{"p":1.0,"text":"From these constraints, we derive model-independent selection rules for decays of double-heavy 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