Diego SANCHEZ

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2018
• Auteurs : A.M. SirunyanArmen TumasyanWolfgang AdamFederico AmbrogiEce AsilarThomas BergauerJohannes BrandstetterErica BrondolinMarko DragicevicJanos EröAlberto Escalante del ValleMartin FlechlRudolf FruehwirthVasile Mihai GheteJosef HrubecManfred JeitlerNatascha KrammerIlse KrätschmerDietrich LikoThomas MadlenerIvan MikulecNavid RadHerbert RohringerJochen SchieckRobert SchöfbeckMarkus SpanringDaniel SpitzbartAnton TaurokWolfgang WaltenbergerJohannes WittmannClaudia-Elisabeth WulzMateusz ZaruckiVladimir ChekhovskyVladimir MossolovJuan Suarez GonzalezEddi A de WolfDavide Di CroceXavier JanssenJasper LauwersMaxim PietersMerijn van de KlundertHans van HaevermaetPierre van MechelenNick van RemortelShimaa Abu ZeidFreya BlekmanJorgen d'HondtIsabelle de BruynJarne de ClercqKevin DerooverGiannis FlourisDenys LontkovskyiSteven LowetteIvan MarchesiniSeth MoortgatLieselotte MoreelsQuentin PythonKirill SkovpenStefaan TavernierWalter van DoninckPetra van MuldersIsis van ParijsDiego BeghinBugra BilinHugues 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• Publié dans Journal of High Energy Physics le 23/10/2020

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Résumé : A search for the pair production of the lightest supersymmetric partner of the top quark $ \left({\tilde{\mathrm{t}}}_1\right) $ is presented. The search focuses on a compressed scenario where the mass difference between the top squark and the lightest supersymmetric particle, often considered to be the lightest neutralino $ \left({\tilde{\upchi}}_1^0\right) $ , is smaller than the mass of the W boson. The proton-proton collision data were recorded by the CMS experiment at a centre-of-mass energy of 13 TeV, and correspond to an integrated luminosity of 35.9 fb$^{−1}$. In this search, two decay modes of the top squark are considered: a four-body decay into a bottom quark, two additional fermions, and a $ {\tilde{\upchi}}_1^0 $ , and a decay via an intermediate chargino. Events are selected using the presence of a high-momentum jet, significant missing transverse momentum, and a low transverse momentum electron or muon. Two analysis techniques are used, targeting different decay modes of the $ {\tilde{\mathrm{t}}}_1 $ : a sequential selection and a multivariate technique. No evidence for the production of top squarks is found, and mass limits at 95% confidence level are set that reach up to 560 GeV, depending on the $ m\left({\tilde{\mathrm{t}}}_1\right)-m\left({\tilde{\upchi}}_1^0\right) $ mass difference and the decay mode.

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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2018
• Auteurs : A.M. SirunyanArmen TumasyanWolfgang AdamFederico AmbrogiEce AsilarThomas BergauerJohannes BrandstetterErica BrondolinMarko DragicevicJanos EröMartin FlechlMarkus FriedlRudolf FruehwirthVasile Mihai GheteJohannes GrossmannJosef HrubecManfred JeitlerAxel KönigNatascha KrammerIlse KrätschmerDietrich LikoThomas MadlenerIvan MikulecElias PreeDinyar RabadyNavid RadHerbert RohringerJochen SchieckRobert SchöfbeckMarkus SpanringDaniel SpitzbartJosef StraussWolfgang WaltenbergerJohannes WittmannClaudia-Elisabeth WulzMateusz ZaruckiVladimir ChekhovskyVladimir MossolovJuan Suarez GonzalezEddi A de WolfDavide Di CroceXavier JanssenJasper LauwersMerijn van de KlundertHans van HaevermaetPierre van MechelenNick van RemortelShimaa Abu ZeidFreya BlekmanJorgen d'HondtIsabelle de BruynJarne de ClercqKevin DerooverGiannis FlourisDenys LontkovskyiSteven LowetteSeth MoortgatLieselotte MoreelsAnnik OlbrechtsQuentin PythonKirill SkovpenStefaan TavernierWalter van DoninckPetra van MuldersIsis van ParijsHugues 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• Publié dans Phys.Lett.B le 31/10/2025

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Résumé : Results are presented from a search for supersymmetry in events with a single electron or muon and hadronic jets. The data correspond to a sample of proton–proton collisions at s=13TeV with an integrated luminosity of 35.9 fb−1 , recorded in 2016 by the CMS experiment. A number of exclusive search regions are defined according to the number of jets, the number of b -tagged jets, the scalar sum of the transverse momenta of the jets, and the scalar sum of the missing transverse momentum and the transverse momentum of the lepton. Standard model background events are reduced significantly by requiring a large azimuthal angle between the direction of the lepton and of the reconstructed W boson, computed under the hypothesis that all of the missing transverse momentum in the event arises from a neutrino produced in the leptonic decay of the W boson. The numbers of observed events are consistent with the expectations from standard model processes, and the results are used to set lower limits on supersymmetric particle masses in the context of two simplified models of gluino pair production. In the first model, where each gluino decays to a top quark–antiquark pair and a neutralino, gluino masses up to 1.8 TeV are excluded at the 95% CL. The second model considers a three-body decay to a light quark–antiquark pair and a chargino, which subsequently decays to a W boson and a neutralino. In this model, gluinos are excluded up to 1.9 TeV.

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