Search for top squark pair production in compressed-mass-spectrum scenarios in proton- proton collisions at √s = 8 TeV using the α_T variable

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dc.contributor.author CMS Collaboration
dc.contributor.author Charaf, O.
dc.contributor.author Cooper, S.I.
dc.contributor.author Henderson, C.
dc.contributor.author Rumerio, P.
dc.date.accessioned 2022-08-02T15:16:20Z
dc.date.available 2022-08-02T15:16:20Z
dc.date.issued 2017
dc.identifier.citation Khachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Erö, J., Flechl, M., Friedl, M., Frühwirth, R., Ghete, V. M., Hartl, C., Hörmann, N., Hrubec, J., Jeitler, M., König, A., … Woods, N. (2017). Search for top squark pair production in compressed-mass-spectrum scenarios in proton–proton collisions at s=8 TeV using the αT variable. In Physics Letters B (Vol. 767, pp. 403–430). Elsevier BV. https://doi.org/10.1016/j.physletb.2017.02.007 en_US
dc.identifier.uri https://ir.ua.edu/handle/123456789/8928
dc.description.abstract An inclusive search is performed for supersymmetry in final states containing jets and an apparent imbalance in transverse momentum, \(\overrightarrow{p}_{T}^{miss}\), due to the production of unobserved weakly interacting particles in pp collisions at a centre-of-mass energy of 8 TeV. The data, recorded with the CMS detector at the CERN LHC, correspond to an integrated luminosity of 18.5 fb⁻¹. The dimensionless kinematic variable \(α_{T}\) is used to discriminate between events with genuine \(\overrightarrow{p}_{T}^{miss}\) associated with unobserved particles and spurious values of \(\overrightarrow{p}_{T}^{miss}\) arising from jet energy mismeasurements. No excess of event yields above the expected standard model backgrounds is observed. The results are interpreted in terms of constraints on the parameter space of several simplified models of supersymmetry that assume the pair production of top squarks. The search provides sensitivity to a broad range of top squark (\(\tilde{t}\)) decay modes, including the two-body decay \(\tilde{t} \to c\tilde{\chi}_{1}^{0}\), where c is a charm quark and \(\tilde{\chi}_{1}^{0}\) is the lightest neutralino, as well as the four-body decay \(\tilde{t} \to bf\overline{f}\prime\tilde{\chi}_{1}^{0}\), where b is a bottom quark and \(f\) and \(\overline{f}\prime\) are fermions produced in the decay of an intermediate off-shell W boson. These modes dominate in scenarios in which the top squark and lightest neutralino are nearly degenerate in mass. For these modes, top squarks with masses as large as 260 and 225 GeV are excluded, respectively, for the two- and four-body decays. en_US
dc.description.uri https://doi.org/10.1016/j.physletb.2017.02.007
dc.format.mimetype application/pdf
dc.language English
dc.rights.uri http://creativecommons.org/licenses/by/3.0/
dc.subject CMS en_US
dc.subject Physics en_US
dc.subject SUSY en_US
dc.subject Jets en_US
dc.subject Missing transverse momentum en_US
dc.subject AlphaT en_US
dc.title Search for top squark pair production in compressed-mass-spectrum scenarios in proton- proton collisions at √s = 8 TeV using the α_T variable en_US
dc.type text


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