Cargando…

Search for supersymmetry with a compressed mass spectrum in events with a soft $\tau$ lepton, a highly energetic jet, and large missing transverse momentum in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$

The first search for supersymmetry in events with one soft tau lepton, one energetic jet from initial state radiation, and transverse momentum imbalance is presented. These event signatures are consistent with those from supersymmetric models exhibiting co-annihilation between the scalar tau lepton...

Descripción completa

Detalles Bibliográficos
Autor principal: CMS Collaboration
Publicado: 2019
Materias:
Acceso en línea:http://cds.cern.ch/record/2684821
_version_ 1780963354915897344
author CMS Collaboration
author_facet CMS Collaboration
author_sort CMS Collaboration
collection CERN
description The first search for supersymmetry in events with one soft tau lepton, one energetic jet from initial state radiation, and transverse momentum imbalance is presented. These event signatures are consistent with those from supersymmetric models exhibiting co-annihilation between the scalar tau lepton ($\tilde{\tau}$) and the lightest neutralino ($\tilde\chi^{0}_{1}$) that could generate the observed relic density of dark matter. The data correspond to an integrated luminosity of $77.2~\mathrm{fb}^{-1}$ of proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$ collected with the CMS detector at the CERN LHC in 2016 and 2017. The results are interpreted considering a supersymmetric scenario with a small mass difference ($\Delta m$) between the chargino ($\tilde{\chi}^{\pm}_{1}$) or the next-to-lightest neutralino ($\tilde{\chi}^{0}_{2}$), and the lightest neutralino. The mass of the $\tilde{\tau}$ is defined as the average of the $\tilde\chi^{\pm}_{1}$/$\tilde\chi^{0}_{2}$ and $\tilde{\chi}^{0}_{1}$ masses. The data are found to be consistent with the standard model background predictions. Upper limits at $95\%$ confidence level are set on the $\tilde{\chi}^{\pm}_{1}$, $\tilde\chi^{0}_{2}$, and $\tilde{\tau}$ production cross sections for $\Delta{m}(\tilde{\chi}^{\pm}_{1}, \tilde\chi^{0}_{1}) = 50~\mathrm{GeV}$, resulting in a lower mass limit of $290~\mathrm{GeV}$ on the mass of the $\tilde\chi^{\pm}_{1}$/$\tilde\chi^{0}_{2}$, which is the most stringent to date.
id cern-2684821
institution Organización Europea para la Investigación Nuclear
publishDate 2019
record_format invenio
spelling cern-26848212019-10-03T20:03:55Zhttp://cds.cern.ch/record/2684821CMS CollaborationSearch for supersymmetry with a compressed mass spectrum in events with a soft $\tau$ lepton, a highly energetic jet, and large missing transverse momentum in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$Particle Physics - ExperimentThe first search for supersymmetry in events with one soft tau lepton, one energetic jet from initial state radiation, and transverse momentum imbalance is presented. These event signatures are consistent with those from supersymmetric models exhibiting co-annihilation between the scalar tau lepton ($\tilde{\tau}$) and the lightest neutralino ($\tilde\chi^{0}_{1}$) that could generate the observed relic density of dark matter. The data correspond to an integrated luminosity of $77.2~\mathrm{fb}^{-1}$ of proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$ collected with the CMS detector at the CERN LHC in 2016 and 2017. The results are interpreted considering a supersymmetric scenario with a small mass difference ($\Delta m$) between the chargino ($\tilde{\chi}^{\pm}_{1}$) or the next-to-lightest neutralino ($\tilde{\chi}^{0}_{2}$), and the lightest neutralino. The mass of the $\tilde{\tau}$ is defined as the average of the $\tilde\chi^{\pm}_{1}$/$\tilde\chi^{0}_{2}$ and $\tilde{\chi}^{0}_{1}$ masses. The data are found to be consistent with the standard model background predictions. Upper limits at $95\%$ confidence level are set on the $\tilde{\chi}^{\pm}_{1}$, $\tilde\chi^{0}_{2}$, and $\tilde{\tau}$ production cross sections for $\Delta{m}(\tilde{\chi}^{\pm}_{1}, \tilde\chi^{0}_{1}) = 50~\mathrm{GeV}$, resulting in a lower mass limit of $290~\mathrm{GeV}$ on the mass of the $\tilde\chi^{\pm}_{1}$/$\tilde\chi^{0}_{2}$, which is the most stringent to date.CMS-PAS-SUS-19-002oai:cds.cern.ch:26848212019
spellingShingle Particle Physics - Experiment
CMS Collaboration
Search for supersymmetry with a compressed mass spectrum in events with a soft $\tau$ lepton, a highly energetic jet, and large missing transverse momentum in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$
title Search for supersymmetry with a compressed mass spectrum in events with a soft $\tau$ lepton, a highly energetic jet, and large missing transverse momentum in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$
title_full Search for supersymmetry with a compressed mass spectrum in events with a soft $\tau$ lepton, a highly energetic jet, and large missing transverse momentum in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$
title_fullStr Search for supersymmetry with a compressed mass spectrum in events with a soft $\tau$ lepton, a highly energetic jet, and large missing transverse momentum in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$
title_full_unstemmed Search for supersymmetry with a compressed mass spectrum in events with a soft $\tau$ lepton, a highly energetic jet, and large missing transverse momentum in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$
title_short Search for supersymmetry with a compressed mass spectrum in events with a soft $\tau$ lepton, a highly energetic jet, and large missing transverse momentum in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$
title_sort search for supersymmetry with a compressed mass spectrum in events with a soft $\tau$ lepton, a highly energetic jet, and large missing transverse momentum in proton-proton collisions at $\sqrt{s}=13~\mathrm{tev}$
topic Particle Physics - Experiment
url http://cds.cern.ch/record/2684821
work_keys_str_mv AT cmscollaboration searchforsupersymmetrywithacompressedmassspectrumineventswithasofttauleptonahighlyenergeticjetandlargemissingtransversemomentuminprotonprotoncollisionsatsqrts13mathrmtev