{"paper":{"title":"Flavorful leptoquarks at the LHC and beyond: Spin 1","arxiv_id":"2103.12724","primary_cat":"hep-ph","submitted_at":"2021-03-23T17:48:47+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":0.95,"id":"s0","own":false,"role":"background","text":"Evidence for electron-muon universality violation that has been revealed in $b\\to s \\ell\\ell$ transitions in the observables $R_{K,K^*}$ by the LHCb Collaboration can be explained with spin-1 leptoquarks in $SU(2)_L$ singlet $V_1$ or triplet $V_3$ representations in the ${\\cal{O}}(1-10)$ TeV range.","hedge":{"p":0.55,"label":"asserted"},"own_p":0.13,"main_claim_p":0.33,"quantitative":true,"quantitative_p":0.96,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.02,"background":0.95,"limitation":0.0,"future_work":0.0,"contribution":0.01,"interpretation":0.02}},{"i":1,"p":1.0,"id":"s1","own":true,"role":"contribution","text":"We explore the sensitivity of the high luminosity LHC (HL-LHC) and future proton-proton colliders to $V_1$ and $V_3$ in the parameter space connected to $R_{K,K^*}$-data.","hedge":{"p":0.73,"label":"asserted"},"own_p":0.8,"main_claim_p":0.05,"quantitative":false,"quantitative_p":0.08,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":1.0,"interpretation":0.0}},{"i":2,"p":0.66,"id":"s2","own":true,"role":"method","text":"We consider pair production and single production in association with muons in different flavor benchmarks.","hedge":{"p":0.73,"label":"asserted"},"own_p":0.81,"main_claim_p":0.03,"quantitative":false,"quantitative_p":0.07,"role_probabilities":{"gap":0.0,"method":0.66,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.34,"interpretation":0.0}},{"i":3,"p":0.99,"id":"s3","own":true,"role":"result","text":"Reinterpreting a recent ATLAS search for scalar leptoquarks decaying to $b \\mu$ and $j \\mu$, we extract improved limits for the leptoquark masses: For gauge boson-type leptoquarks ($\\kappa=1$) we obtain $M_{V_1}> 1.9$ TeV, $M_{V_1}> 1.9$ TeV, and $M_{V_1}> 1.7$ TeV for leptoquarks decaying predominantly according to hierarchical, flipped and democratic quark flavor structure, respectively.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.9,"main_claim_p":0.13,"quantitative":true,"quantitative_p":0.99,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.99,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.01,"interpretation":0.0}},{"i":4,"p":0.64,"id":"s4","own":true,"role":"method","text":"Future sensitivity projections based on extrapolations of existing ATLAS and CMS searches are worked out.","hedge":{"p":0.92,"label":"asserted"},"own_p":0.86,"main_claim_p":0.04,"quantitative":false,"quantitative_p":0.05,"role_probabilities":{"gap":0.0,"method":0.64,"result":0.01,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.35,"interpretation":0.0}},{"i":5,"p":1.0,"id":"s5","own":true,"role":"result","text":"We find that for $\\kappa=1$ the mass reach for pair (single) production of $V_1$ can be up to 3 TeV (2.1 TeV) at the HL-LHC and up to 15 TeV (19.9 TeV) at the FCC-hh with $\\sqrt{s}=100$ TeV and $20 \\, \\mbox{ab}^{-1}$.","hedge":{"p":0.97,"label":"asserted"},"own_p":0.93,"main_claim_p":0.25,"quantitative":true,"quantitative_p":0.99,"role_probabilities":{"gap":0.0,"method":0.0,"result":1.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.0}},{"i":6,"p":1.0,"id":"s6","own":true,"role":"result","text":"The mass limits and reach for the triplet $V_3$ are similar or higher, depending on flavor.","hedge":{"p":0.97,"label":"asserted"},"own_p":0.82,"main_claim_p":0.09,"quantitative":true,"quantitative_p":0.93,"role_probabilities":{"gap":0.0,"method":0.0,"result":1.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.0}},{"i":7,"p":0.54,"id":"s7","own":false,"role":"interpretation","text":"While there is the exciting possibility that leptoquarks addressing the $R_{K,K^*}$-anomalies are observed at the LHC, to fully cover the parameter space $pp$-collisions beyond the LHC-energies are needed.","hedge":{"p":0.68,"label":"hedged_possibility"},"own_p":0.24,"main_claim_p":0.55,"quantitative":false,"quantitative_p":0.12,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.01,"background":0.0,"limitation":0.17,"future_work":0.28,"contribution":0.0,"interpretation":0.54}}]},"compiled":{"main_claim":{"p":0.94,"text":"While there is the exciting possibility that leptoquarks addressing the $R_{K,K^*}$-anomalies are observed at the LHC, to fully cover the parameter space $pp$-collisions beyond the LHC-energies are needed.","location":"abstract s7","hedge_strength":{"p":0.68,"label":"hedged possibility"}},"provenance":{"route":{"via":"TypeSafe API","model":"classifier-1.13.0","endpoint":"https://api.typesafe.ai/v1/systemone","provider":"TypeSafe"},"packing":"one request per 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