Publication:
A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb?1 of pp collision data collected by the ATLAS detector

cris.lastimport.scopus2026-03-17T18:53:46Z
datacite.subject.fosNatural sciences::Physical sciences::Particles and fields physics
dc.contributor.authorG. Aad
dc.contributor.authorB. Abbott
dc.contributor.authorK. Abeling
dc.contributor.authorN. J. Abicht
dc.contributor.authorS. H. Abidi
dc.contributor.authorA. Aboulhorma
dc.contributor.authorH. Abramowicz
dc.contributor.authorH. Abreu
dc.contributor.authorY. Abulaiti
dc.contributor.authorB. S. Acharya
dc.contributor.authorC. Adam Bourdarios
dc.contributor.authorL. Adamczyk
dc.contributor.authorS. V. Addepalli
dc.contributor.authorM. J. Addison
dc.contributor.authorJ. Adelman
dc.contributor.authorA. Adiguzel
dc.contributor.authorT. Adye
dc.contributor.authorA. A. Affolder
dc.contributor.authorY. Afik
dc.contributor.authorM. N. Agaras
dc.date.accessioned2026-01-13T18:52:18Z
dc.date.available2026-01-13T18:52:18Z
dc.date.issued2024-07-26
dc.description.abstractThis paper presents a search for top-squark pair production in final states with a top quark, a charm quark and missing transverse momentum. The data were collected with the ATLAS detector during LHC Run 2 and correspond to an integrated luminosity of 139 fb⁻¹ of proton–proton collisions at a centre-of-mass energy of √s = 13 TeV. The analysis is motivated by an extended Minimal Supersymmetric Standard Model featuring a non-minimal flavour violation in the second- and third-generation squark sector. The top squark in this model has two possible decay modes, either t̃₁ → t χ̃⁰₁ or t̃₁ → c χ̃⁰₁, where the χ̃⁰₁ is undetected. The analysis is optimised assuming that both of the decay modes are equally probable, leading to the most likely final state of t c + Eₜᵐⁱˢˢ. Good agreement is found between the Standard Model expectation and the data in the search regions. Exclusion limits at 95% confidence level are obtained in the m(t̃₁) vs. m(χ̃⁰₁) plane and, in addition, limits on the branching ratio of the t̃₁ → c χ̃⁰₁ decay as a function of m(t̃₁) are also produced. Top-squark masses of up to 800 GeV are excluded for scenarios with light neutralinos, and top-squark masses up to 600 GeV are excluded in scenarios where the neutralino and the top squark are almost mass-degenerate.en_US
dc.identifier.doi10.1007/JHEP07(2024)250
dc.identifier.urihttps://cris.usm.cl/handle/123456789/4254
dc.language.isoen_US
dc.publisherSpringer Science and Business Media LLC
dc.relation.ispartofJournal of High Energy Physics
dc.relation.issn1029-8479
dc.rightsAttribution 4.0 Internationalen
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/
dc.subjectTop squark
dc.subjectSupersymmetry
dc.subjectR-parity violation
dc.subjectHadron-hadron collisions
dc.subjectJets
dc.subjectMissing transverse momentum
dc.subjectBeyond Standard Model physics
dc.subjectATLAS experiment
dc.subjectLarge Hadron Collider
dc.subject.ods4 Educación de calidad
dc.subject.ods9 Industria, innovación e infraestructura
dc.subject.ods17 Alianzas para lograr los objetivos
dc.titleA search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb?1 of pp collision data collected by the ATLAS detector
dc.typetext::journal::journal article::research article
dspace.entity.typePublication
oaire.citation.issue7
oaire.citation.volume2024

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