{"paper":{"title":"A symmetry for $\\epsilon_K$","arxiv_id":"1704.08704","primary_cat":"hep-ph","submitted_at":"2017-04-27T18:01:43+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":0.77,"id":"s0","own":true,"role":"contribution","text":"We show a symmetry that, in the context of a composite Higgs with anarchic flavor, can suppress the dominant CP violating contributions to $K-\\bar K$ mixing.","hedge":{"p":0.8,"label":"asserted"},"own_p":0.94,"main_claim_p":0.87,"quantitative":false,"quantitative_p":0.11,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.23,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.77,"interpretation":0.0}},{"i":1,"p":0.48,"id":"s1","own":false,"role":"method","text":"Based on previous extensions of SU(3)$_c$, we consider the case in which the composite sector has a global SU(6) symmetry, spontaneously broken to a subgroup containing SU(3)$\\times$SU(3).","hedge":{"p":0.8,"label":"asserted"},"own_p":0.31,"main_claim_p":0.04,"quantitative":false,"quantitative_p":0.25,"role_probabilities":{"gap":0.0,"method":0.48,"result":0.0,"background":0.34,"limitation":0.0,"future_work":0.0,"contribution":0.18,"interpretation":0.0}},{"i":2,"p":0.8,"id":"s2","own":true,"role":"result","text":"We show that the interactions with the Standard Model can spontaneously break the remaining symmetry to the diagonal subgroup, identified with the group of color interactions, and naturally suppress $\\epsilon_K$.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.87,"main_claim_p":0.37,"quantitative":false,"quantitative_p":0.05,"role_probabilities":{"gap":0.0,"method":0.02,"result":0.8,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.17,"interpretation":0.01}},{"i":3,"p":0.58,"id":"s3","own":false,"role":"method","text":"We consider this scenario in the context of the Minimal Composite Higgs Model based on SO(5)/SO(4) for the electroweak sector.","hedge":{"p":0.81,"label":"asserted"},"own_p":0.45,"main_claim_p":0.04,"quantitative":false,"quantitative_p":0.16,"role_probabilities":{"gap":0.0,"method":0.58,"result":0.0,"background":0.34,"limitation":0.0,"future_work":0.0,"contribution":0.08,"interpretation":0.0}},{"i":4,"p":0.97,"id":"s4","own":true,"role":"method","text":"By working in the framework of 2-site models, we compute the scalar potential, determine the conditions for a successful breaking of the symmetries and calculate the spectrum of lightest states.","hedge":{"p":0.91,"label":"asserted"},"own_p":0.95,"main_claim_p":0.04,"quantitative":false,"quantitative_p":0.22,"role_probabilities":{"gap":0.0,"method":0.97,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.03,"interpretation":0.0}},{"i":5,"p":1.0,"id":"s5","own":true,"role":"result","text":"We find that $\\epsilon_K$ can be suppressed and the top mass reproduced for a large region of the parameter space where 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