Monojet signatures from gluino and squark decays

Abstract We study the monojet and dijet channels at the LHC as a tool for searching for squarks and gluinos. We consider two separate R-parity conserving supersymmetric scenarios. In the first scenario we postulate a large mass hierarchy between squarks ( q ~ $$ \overset{\sim }{q} $$ ) and winos ( W...

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Main Authors: Iñaki Lara, Trygve Buanes, Rafał Masełek, Mihoko M. Nojiri, Krzysztof Rolbiecki, Kazuki Sakurai
Format: Article
Language:English
Published: SpringerOpen 2022-10-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP10(2022)150
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author Iñaki Lara
Trygve Buanes
Rafał Masełek
Mihoko M. Nojiri
Krzysztof Rolbiecki
Kazuki Sakurai
author_facet Iñaki Lara
Trygve Buanes
Rafał Masełek
Mihoko M. Nojiri
Krzysztof Rolbiecki
Kazuki Sakurai
author_sort Iñaki Lara
collection DOAJ
description Abstract We study the monojet and dijet channels at the LHC as a tool for searching for squarks and gluinos. We consider two separate R-parity conserving supersymmetric scenarios. In the first scenario we postulate a large mass hierarchy between squarks ( q ~ $$ \overset{\sim }{q} $$ ) and winos ( W ~ $$ \overset{\sim }{W} $$ ), and wino-like neutralino is assumed to be the lightest supersymmetric particle (LSP). The associated squark-wino production, pp → q ~ W ~ $$ \overset{\sim }{q}\overset{\sim }{W} $$ , then leads to a monojet-like signature, where the high p T jet is originated from the squark decay, q ~ $$ \overset{\sim }{q} $$ → q + W ~ $$ \overset{\sim }{W} $$ . We demonstrate that this associated production, as well as the pp → W ~ W ~ $$ \overset{\sim }{W}\overset{\sim }{W} $$ + jets production, have a significant impact on the exclusion limit in the squark-neutralino mass plane. The second scenario postulates that the lighter of the squark and gluino is only a few GeV heavier than the LSP neutralino. The associated squark-gluino production, pp → q ~ g ~ $$ \overset{\sim }{q}\overset{\sim }{g} $$ , then leads to a distinctive monojet signature, where the high p T jet is produced from the decay of the heavier coloured particle into the lighter one ( q ~ $$ \overset{\sim }{q} $$ → q+ g ~ $$ \overset{\sim }{g} $$ for m q ~ $$ {m}_{\tilde{q}} $$ > m g ~ $$ {m}_{\tilde{g}} $$ and g ~ $$ \overset{\sim }{g} $$ → q+ q ~ $$ \overset{\sim }{q} $$ for m g ~ $$ {m}_{\tilde{g}} $$ > m q ~ $$ {m}_{\tilde{q}} $$ ). The lighter coloured particle is effectively regarded as an invisible particle since the decay products are soft due to the approximate mass degeneracy. We recast existing monojet and dijet analyses and find a non-trivial exclusion limit in the squark-gluino mass plane in this scenario.
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spelling doaj.art-2fa3575e47e24aba8ba202e50a89a9502022-12-22T02:37:22ZengSpringerOpenJournal of High Energy Physics1029-84792022-10-0120221012210.1007/JHEP10(2022)150Monojet signatures from gluino and squark decaysIñaki Lara0Trygve Buanes1Rafał Masełek2Mihoko M. Nojiri3Krzysztof Rolbiecki4Kazuki Sakurai5Institute of Theoretical Physics, Faculty of Physics, University of WarsawWestern Norway University of Applied SciencesInstitute of Theoretical Physics, Faculty of Physics, University of WarsawTheory Center, IPNS, KEKInstitute of Theoretical Physics, Faculty of Physics, University of WarsawInstitute of Theoretical Physics, Faculty of Physics, University of WarsawAbstract We study the monojet and dijet channels at the LHC as a tool for searching for squarks and gluinos. We consider two separate R-parity conserving supersymmetric scenarios. In the first scenario we postulate a large mass hierarchy between squarks ( q ~ $$ \overset{\sim }{q} $$ ) and winos ( W ~ $$ \overset{\sim }{W} $$ ), and wino-like neutralino is assumed to be the lightest supersymmetric particle (LSP). The associated squark-wino production, pp → q ~ W ~ $$ \overset{\sim }{q}\overset{\sim }{W} $$ , then leads to a monojet-like signature, where the high p T jet is originated from the squark decay, q ~ $$ \overset{\sim }{q} $$ → q + W ~ $$ \overset{\sim }{W} $$ . We demonstrate that this associated production, as well as the pp → W ~ W ~ $$ \overset{\sim }{W}\overset{\sim }{W} $$ + jets production, have a significant impact on the exclusion limit in the squark-neutralino mass plane. The second scenario postulates that the lighter of the squark and gluino is only a few GeV heavier than the LSP neutralino. The associated squark-gluino production, pp → q ~ g ~ $$ \overset{\sim }{q}\overset{\sim }{g} $$ , then leads to a distinctive monojet signature, where the high p T jet is produced from the decay of the heavier coloured particle into the lighter one ( q ~ $$ \overset{\sim }{q} $$ → q+ g ~ $$ \overset{\sim }{g} $$ for m q ~ $$ {m}_{\tilde{q}} $$ > m g ~ $$ {m}_{\tilde{g}} $$ and g ~ $$ \overset{\sim }{g} $$ → q+ q ~ $$ \overset{\sim }{q} $$ for m g ~ $$ {m}_{\tilde{g}} $$ > m q ~ $$ {m}_{\tilde{q}} $$ ). The lighter coloured particle is effectively regarded as an invisible particle since the decay products are soft due to the approximate mass degeneracy. We recast existing monojet and dijet analyses and find a non-trivial exclusion limit in the squark-gluino mass plane in this scenario.https://doi.org/10.1007/JHEP10(2022)150Dark Matter at CollidersSupersymmetryJets and Jet Substructure
spellingShingle Iñaki Lara
Trygve Buanes
Rafał Masełek
Mihoko M. Nojiri
Krzysztof Rolbiecki
Kazuki Sakurai
Monojet signatures from gluino and squark decays
Journal of High Energy Physics
Dark Matter at Colliders
Supersymmetry
Jets and Jet Substructure
title Monojet signatures from gluino and squark decays
title_full Monojet signatures from gluino and squark decays
title_fullStr Monojet signatures from gluino and squark decays
title_full_unstemmed Monojet signatures from gluino and squark decays
title_short Monojet signatures from gluino and squark decays
title_sort monojet signatures from gluino and squark decays
topic Dark Matter at Colliders
Supersymmetry
Jets and Jet Substructure
url https://doi.org/10.1007/JHEP10(2022)150
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AT krzysztofrolbiecki monojetsignaturesfromgluinoandsquarkdecays
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