{"arxiv_id":"hep-ph/9902431","incoming":{"papers":6,"sentences":20,"groups":[{"kind":"contests","label":"Contests it","papers":2,"sentences":4,"quotes":[{"arxiv_id":"2303.18002","title":"Are we close to solving the puzzle of weak radiative hyperon decays?","url":"/paper/2303.18002","section":"Introduction","sentence":"None of the previous predictions in the pole models (PM) [ref] , the vector-dominance model (VDM) [ref] , the chiral perturbation theory ($χ$PT) [ref] , the broken SU(3) model [ref] , the quark model (QM) [ref] and the non-relativistic constituent quark model (NRCQM) [ref] can describe the new data.","intent_p":0.55,"contests_p":0.92},{"arxiv_id":"2206.11773","title":"Weak radiative hyperon decays in covariant baryon chiral perturbation theory","url":"/paper/2206.11773","section":"Introduction","sentence":"For instance, the predicted decay parameters for $Ξ^0→Σ^0γ$ and $Ξ^0→Λγ$ in Ref. [ref] are 0.15 and 0.46, respectively, in sharp conflict with the latest experimental data.","intent_p":0.8,"contests_p":0.95}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2206.11773","title":"Weak radiative hyperon decays in covariant baryon chiral perturbation theory","url":"/paper/2206.11773","section":"Introduction","sentence":"Furthermore, we note that the results of the pole model (PM I) [ref] and $χ$PT at tree level [ref] are relatively closer to the new BESIII data.","intent_p":0.98,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2604.00646","title":"Hyperon non-leptonic decays in relativistic Chiral Perturbation Theory with resonances","url":"/paper/2604.00646","section":"Conclusion and outlook","sentence":"Certainly, our results give further credit to the suggestion of Ref. [ref] that such states are of crucial importance to understand the weak radiative decays of hyperons.","intent_p":0.98,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":2,"sentences":2,"quotes":[{"arxiv_id":"2206.11773","title":"Weak radiative hyperon decays in covariant baryon chiral perturbation theory","url":"/paper/2206.11773","section":"Introduction","sentence":"For a short introduction to these three methods, see, e.g., Ref. [ref] . $χPT$ has been applied to study the WRHDs in the covariant formulation [ref] and the heavy baryon formulation [ref] up to one-loop order and at tree level but considering the contribution of heavier resonances [ref] .","intent_p":0.94,"contests_p":null},{"arxiv_id":"2608.03248","title":"Unraveling weak radiative hyperon decays with broken flavor symmetry","url":"/paper/2608.03248","section":"Introduction","sentence":"Despite their simple two-body kinematics, these decays have long posed significant challenges to both theory and experiment [ref] .","intent_p":0.95,"contests_p":null}]}],"unlabelled_sentences":12},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/hep-ph/9902431"}}