{"paper":{"title":"p p -> J/psi+Upsilon+X as a clean probe to the quarkonium production mechanism","arxiv_id":"1006.3846","primary_cat":"hep-ph","submitted_at":"2010-06-19T07:11:24+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. 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respectively.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.79,"main_claim_p":0.79,"quantitative":true,"quantitative_p":0.54,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.88,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.11,"interpretation":0.01}},{"i":1,"p":0.57,"id":"s1","own":true,"role":"result","text":"With the integrated luminosity ~ 100 fb^{-1} at the center-of-momentum energy sqrt{s}=14 TeV we expect that approximately 1900 p p -> J/psi+Upsilon+X events can be observed at the CERN Large Hadron Collider by tagging muon pairs, which are enough to probe to the color-octet mechanism.","hedge":{"p":0.54,"label":"hedged_possibility"},"own_p":0.51,"main_claim_p":0.15,"quantitative":true,"quantitative_p":0.99,"role_probabilities":{"gap":0.0,"method":0.23,"result":0.57,"background":0.0,"limitation":0.0,"future_work":0.09,"contribution":0.08,"interpretation":0.03}},{"i":2,"p":0.68,"id":"s2","own":false,"role":"interpretation","text":"The forthcoming measurement may provide a useful constraint to resolve the decade-old puzzle for the polarization of prompt J/psi at the Fermilab Tevatron.","hedge":{"p":1.0,"label":"hedged_possibility"},"own_p":0.06,"main_claim_p":0.09,"quantitative":false,"quantitative_p":0.08,"role_probabilities":{"gap":0.01,"method":0.0,"result":0.0,"background":0.03,"limitation":0.0,"future_work":0.26,"contribution":0.01,"interpretation":0.68}},{"i":3,"p":0.99,"id":"s3","own":false,"role":"interpretation","text":"If corresponding measured rate is significantly less than the prediction, it may imply that the current values for the color-octet matrix elements are overestimated.","hedge":{"p":1.0,"label":"hedged_possibility"},"own_p":0.06,"main_claim_p":0.07,"quantitative":true,"quantitative_p":0.74,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.01,"contribution":0.0,"interpretation":0.99}}]},"compiled":{"main_claim":{"p":0.99,"text":"We report that, 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quarkonium-production processes, the production rate for p p -> J/psi+Upsilon+X dominantly depends on two not well-known long-distance nonrelativistic QCD matrix elements, <O_8^{J/psi}(^3S_1)> and <O_8^{Upsilon}(^3S_1)> at leading order in the strong coupling constant, which account for the transition probabilities of the color-octet spin-triplet heavy-quark-antiquark pairs c\\bar{c}_8(^3S_1) -> J/psi and b\\bar{b}_8(^3S_1) -> Upsilon, respectively.","location":"abstract s0"}},"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":4,"sentences_in_abstract":4},"measured_accuracy":{"url":"https://pith.science/accuracy","measured_on":"2026-10-02","method":"two independent model families labelled a fresh random sample 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