{"paper":{"title":"Explaining the $R_{K^{(*)}}$ anomalies and the CDF $M_W$ in Flavorful Top Seesaw Models with Gauged $U(1)_{L(-R)}$","arxiv_id":"2210.13402","primary_cat":"hep-ph","submitted_at":"2022-10-24T16:57:08+00:00","version_compiled":"v3"},"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. 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$U(2)_L$.","hedge":{"p":0.97,"label":"asserted"},"own_p":0.75,"main_claim_p":0.04,"quantitative":false,"quantitative_p":0.26,"role_probabilities":{"gap":0.0,"method":0.24,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.76,"interpretation":0.0}},{"i":2,"p":0.61,"id":"s2","own":false,"role":"method","text":"The symmetry is partially gauged such that the breaking introduces not only a composite Higgs doublet but also a TeV-scale $Z'$ boson.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.43,"main_claim_p":0.07,"quantitative":false,"quantitative_p":0.39,"role_probabilities":{"gap":0.0,"method":0.61,"result":0.02,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.37,"interpretation":0.0}},{"i":3,"p":0.62,"id":"s3","own":true,"role":"result","text":"The $U(3)_L/U(2)_L$ Top Seesaw model predicts a light Higgs boson as well as a large top Yukawa coupling.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.5,"main_claim_p":0.05,"quantitative":false,"quantitative_p":0.25,"role_probabilities":{"gap":0.0,"method":0.14,"result":0.62,"background":0.11,"limitation":0.0,"future_work":0.0,"contribution":0.11,"interpretation":0.02}},{"i":4,"p":0.56,"id":"s4","own":false,"role":"method","text":"Additional $U(1)'$ symmetry is gauged such that a flavorful TeV-scale $Z'$ boson is introduced to address the B anomalies.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.49,"main_claim_p":0.09,"quantitative":false,"quantitative_p":0.26,"role_probabilities":{"gap":0.0,"method":0.56,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.44,"interpretation":0.0}},{"i":5,"p":0.48,"id":"s5","own":false,"role":"result","text":"The existence of a heavy vector-like top quark and $Z-Z'$ mixing breaks the custodial symmetry, which predicts a heavier $W$ mass as observed by the CDF collaboration.","hedge":{"p":0.99,"label":"asserted"},"own_p":0.48,"main_claim_p":0.16,"quantitative":false,"quantitative_p":0.46,"role_probabilities":{"gap":0.0,"method":0.02,"result":0.48,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.03,"interpretation":0.47}},{"i":6,"p":0.75,"id":"s6","own":true,"role":"contribution","text":"Two possible candidates for the $U(1)'$ symmetry corresponding to the $Z'$ boson, $U(1)_L$ and $U(1)_{L-R}$, are discussed in detail.","hedge":{"p":0.83,"label":"asserted"},"own_p":0.72,"main_claim_p":0.05,"quantitative":false,"quantitative_p":0.37,"role_probabilities":{"gap":0.0,"method":0.25,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.75,"interpretation":0.0}},{"i":7,"p":0.75,"id":"s7","own":true,"role":"contribution","text":"The parameter space for the models to address both anomalies is presented.","hedge":{"p":0.9,"label":"asserted"},"own_p":0.86,"main_claim_p":0.09,"quantitative":false,"quantitative_p":0.05,"role_probabilities":{"gap":0.0,"method":0.01,"result":0.24,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.75,"interpretation":0.0}},{"i":8,"p":0.86,"id":"s8","own":true,"role":"contribution","text":"The direct searches of the $Z'$ boson from dilepton channels are also studied.","hedge":{"p":0.97,"label":"asserted"},"own_p":0.83,"main_claim_p":0.04,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.14,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.86,"interpretation":0.0}},{"i":9,"p":0.44,"id":"s9","own":true,"role":"interpretation","text":"Based on the assumptions, a TeV-scale $Z'$ boson is still viable and can be probed in the near 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