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Constraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at $\sqrt{s}=13~\mathrm{TeV}$

Many searches for Supersymmetry at the CERN LHC are sensitive to other scenarios of physics beyond the standard model. In this note, the results of a previous search for squarks and gluinos are re-interpreted to constrain models of leptoquark production. Pair production is considered, and both lepto...

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Autor principal: CMS Collaboration
Publicado: 2018
Materias:
Acceso en línea:http://cds.cern.ch/record/2308307
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author CMS Collaboration
author_facet CMS Collaboration
author_sort CMS Collaboration
collection CERN
description Many searches for Supersymmetry at the CERN LHC are sensitive to other scenarios of physics beyond the standard model. In this note, the results of a previous search for squarks and gluinos are re-interpreted to constrain models of leptoquark production. Pair production is considered, and both leptoquarks are assumed to decay to a quark and a neutrino. The search selects jets in association with a transverse momentum imbalance, using the $M_{\mathrm{T2}}$ variable. The analysis uses proton-proton collision data at $\sqrt{s}=13~\mathrm{TeV}$, recorded with the CMS detector at the LHC in 2016 and corresponding to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$. Compared to previous CMS results, both scalar and vector leptoquarks are considered, as well as higher leptoquark mass values, and for the first time, leptoquark decays to a light quark (any single one of u, d, s, or c) and a neutrino are considered. Assuming scalar (vector) leptoquarks decaying with unity branching fraction to a light quark and neutrino, masses below $980~(1790)~\mathrm{GeV}$ are excluded by the observed data. For leptoquarks decaying to a bottom quark and a neutrino, masses below $1100~(1810)~\mathrm{GeV}$ are excluded, while assuming decays to a top quark and a neutrino, masses below $1020~(1780)~\mathrm{GeV}$ are excluded. Vector leptoquarks decaying with a $50\%$ branching fraction to a top quark and a neutrino, and $50\%$ to a bottom quark and tau lepton, have been proposed as an explanation of anomalous flavor physics results. In such a model, we exclude leptoquarks with masses below $1530~\mathrm{GeV}$, placing the most stringent constraint to date.
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spelling cern-23083072019-09-30T06:29:59Zhttp://cds.cern.ch/record/2308307CMS CollaborationConstraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at $\sqrt{s}=13~\mathrm{TeV}$Particle Physics - ExperimentMany searches for Supersymmetry at the CERN LHC are sensitive to other scenarios of physics beyond the standard model. In this note, the results of a previous search for squarks and gluinos are re-interpreted to constrain models of leptoquark production. Pair production is considered, and both leptoquarks are assumed to decay to a quark and a neutrino. The search selects jets in association with a transverse momentum imbalance, using the $M_{\mathrm{T2}}$ variable. The analysis uses proton-proton collision data at $\sqrt{s}=13~\mathrm{TeV}$, recorded with the CMS detector at the LHC in 2016 and corresponding to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$. Compared to previous CMS results, both scalar and vector leptoquarks are considered, as well as higher leptoquark mass values, and for the first time, leptoquark decays to a light quark (any single one of u, d, s, or c) and a neutrino are considered. Assuming scalar (vector) leptoquarks decaying with unity branching fraction to a light quark and neutrino, masses below $980~(1790)~\mathrm{GeV}$ are excluded by the observed data. For leptoquarks decaying to a bottom quark and a neutrino, masses below $1100~(1810)~\mathrm{GeV}$ are excluded, while assuming decays to a top quark and a neutrino, masses below $1020~(1780)~\mathrm{GeV}$ are excluded. Vector leptoquarks decaying with a $50\%$ branching fraction to a top quark and a neutrino, and $50\%$ to a bottom quark and tau lepton, have been proposed as an explanation of anomalous flavor physics results. In such a model, we exclude leptoquarks with masses below $1530~\mathrm{GeV}$, placing the most stringent constraint to date.CMS-PAS-SUS-18-001oai:cds.cern.ch:23083072018
spellingShingle Particle Physics - Experiment
CMS Collaboration
Constraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at $\sqrt{s}=13~\mathrm{TeV}$
title Constraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at $\sqrt{s}=13~\mathrm{TeV}$
title_full Constraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at $\sqrt{s}=13~\mathrm{TeV}$
title_fullStr Constraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at $\sqrt{s}=13~\mathrm{TeV}$
title_full_unstemmed Constraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at $\sqrt{s}=13~\mathrm{TeV}$
title_short Constraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at $\sqrt{s}=13~\mathrm{TeV}$
title_sort constraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at $\sqrt{s}=13~\mathrm{tev}$
topic Particle Physics - Experiment
url http://cds.cern.ch/record/2308307
work_keys_str_mv AT cmscollaboration constraintsonmodelsofscalarandvectorleptoquarksdecayingtoaquarkandaneutrinoatsqrts13mathrmtev