{"paper":{"title":"Natural SUSY's Last Hope: R-parity Violation via UDD Operators","arxiv_id":"1301.2336","primary_cat":"hep-ph","submitted_at":"2013-01-10T21:31:52+00:00","version_compiled":"v1"},"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. No sentence in this record was written by a language model.","schema":"pith.compiled-record/v0","status":"compiled","abstract":{"source":"arXiv listing abstract v1","sentences":[{"i":0,"p":0.99,"id":"s0","own":true,"role":"contribution","text":"Here, we give a broad overview of the more natural spectra allowed by the LHC when UDD R-parity violation is allowed.","hedge":{"p":0.67,"label":"asserted"},"own_p":0.74,"main_claim_p":0.19,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.0,"background":0.01,"limitation":0.0,"future_work":0.0,"contribution":0.99,"interpretation":0.0}},{"i":1,"p":0.57,"id":"s1","own":false,"role":"background","text":"Because R-parity violation removes the missing energy signals in colliders, the experimental constraints on the gluino, stops, sbottoms and higgsinos are relatively mild.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.13,"main_claim_p":0.15,"quantitative":false,"quantitative_p":0.36,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.21,"background":0.57,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.22}},{"i":2,"p":0.75,"id":"s2","own":true,"role":"result","text":"We also show that UDD R-parity violation and lepton number conservation can be made consistent with grand unification.","hedge":{"p":0.54,"label":"hedged_possibility"},"own_p":0.83,"main_claim_p":0.21,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.75,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.25,"interpretation":0.0}},{"i":3,"p":0.91,"id":"s3","own":true,"role":"method","text":"This feat is achieved through the product unification, SU(5) X U(3).","hedge":{"p":1.0,"label":"asserted"},"own_p":0.54,"main_claim_p":0.09,"quantitative":false,"quantitative_p":0.12,"role_probabilities":{"gap":0.0,"method":0.91,"result":0.01,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.08,"interpretation":0.0}},{"i":4,"p":0.91,"id":"s4","own":false,"role":"method","text":"In this model, mixing of the SM quarks with additional quark like particles charged under the U(3) generate a UDD R-parity violating operator.","hedge":{"p":0.99,"label":"asserted"},"own_p":0.49,"main_claim_p":0.12,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.91,"result":0.01,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.08,"interpretation":0.0}},{"i":5,"p":0.87,"id":"s5","own":true,"role":"result","text":"Furthermore, these models are also capable of generating a \"natural\" spectra.","hedge":{"p":0.65,"label":"asserted"},"own_p":0.65,"main_claim_p":0.26,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.87,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.12,"interpretation":0.01}},{"i":6,"p":0.88,"id":"s6","own":true,"role":"interpretation","text":"The emergence of these more natural low-scale spectra relies heavily on the fact that the gaugino masses are non-universal, a natural consequence of product unification.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.55,"main_claim_p":0.22,"quantitative":false,"quantitative_p":0.05,"role_probabilities":{"gap":0.0,"method":0.03,"result":0.09,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.88}}]},"compiled":{"main_claim":{"p":0.59,"text":"Furthermore, these models are also capable of generating a \"natural\" spectra.","location":"abstract 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