Show simple item record

dc.contributor.authorTumasyan, A.
dc.contributor.authorAdam, W.
dc.contributor.authorAndrejkovic, J. W.
dc.contributor.authorBergauer, T.
dc.contributor.authorChatterjee, S.
dc.contributor.authorDamanakis, K.
dc.contributor.authorDragicevic, M.
dc.contributor.authorEscalante Del Valle, A.
dc.contributor.authorHussain, P. S.
dc.contributor.authorJeitler, M.
dc.contributor.authorKrammer, N.
dc.contributor.authorLechner, L.
dc.contributor.authorLiko, D.
dc.contributor.authorMikulec, I.
dc.contributor.authorPaulitsch, P.
dc.contributor.authorPitters, F. M.
dc.contributor.authorSchieck, J.
dc.date.accessioned2023-06-20T19:29:11Z
dc.date.available2023-06-20T19:29:11Z
dc.date.issued2023-06-12
dc.identifier.urihttps://hdl.handle.net/1721.1/150926
dc.description.abstractAbstract A search for the pair production of the lightest supersymmetric partner of the top quark, the top squark ( t ~ 1 $$ {\overset{\sim }{\textrm{t}}}_1 $$ ), is presented. The search targets the four-body decay of the t ~ 1 $$ {\overset{\sim }{\textrm{t}}}_1 $$ , which is preferred when the mass difference between the top squark and the lightest supersymmetric particle is smaller than the mass of the W boson. This decay mode consists of a bottom quark, two other fermions, and the lightest neutralino ( χ ~ 1 0 $$ {\overset{\sim }{\chi}}_1^0 $$ ), which is assumed to be the lightest supersymmetric particle. The data correspond to an integrated luminosity of 138 fb−1 of proton-proton collisions at a center-of-mass energy of 13 TeV collected by the CMS experiment at the CERN LHC. Events are selected using the presence of a high-momentum jet, an electron or muon with low transverse momentum, and a significant missing transverse momentum. The signal is selected based on a multivariate approach that is optimized for the difference between m( t ~ 1 $$ {\overset{\sim }{\textrm{t}}}_1 $$ ) and m( χ ~ 1 0 $$ {\overset{\sim }{\chi}}_1^0 $$ ). The contribution from leading background processes is estimated from data. No significant excess is observed above the expectation from standard model processes. The results of this search exclude top squarks at 95% confidence level for masses up to 480 and 700 GeV for m( t ~ 1 $$ {\overset{\sim }{\textrm{t}}}_1 $$ ) − m( χ ~ 1 0 $$ {\overset{\sim }{\chi}}_1^0 $$ ) = 10 and 80 GeV, respectively.en_US
dc.publisherSpringer Berlin Heidelbergen_US
dc.relation.isversionofhttps://doi.org/10.1007/JHEP06(2023)060en_US
dc.rightsCreative Commons Attributionen_US
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/en_US
dc.sourceSpringer Berlin Heidelbergen_US
dc.titleSearch for top squarks in the four-body decay mode with single lepton final states in proton-proton collisions at s $$ \sqrt{s} $$ = 13 TeVen_US
dc.typeArticleen_US
dc.identifier.citationJournal of High Energy Physics. 2023 Jun 12;2023(6):60en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physics
dc.identifier.mitlicensePUBLISHER_CC
dc.eprint.versionFinal published versionen_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dc.date.updated2023-06-18T03:10:30Z
dc.language.rfc3066en
dc.rights.holderThe Author(s)
dspace.embargo.termsN
dspace.date.submission2023-06-18T03:10:29Z
mit.licensePUBLISHER_CC
mit.metadata.statusAuthority Work and Publication Information Neededen_US


Files in this item

Thumbnail

This item appears in the following Collection(s)

Show simple item record