Search for top squark pair production using dilepton final states in pp collision data collected at s = 13 TeV.
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MariniC McginnC MironovS NarayananX NiuC PausD RankinC RolandG RolandZ ShiG S F StephansK SumorokK TatarD VelicanuJ WangT W WangZ WangB WyslouchR M ChatterjeeA EvansS GutsP HansenJ HiltbrandSh JainM KrohnY KubotaZ LeskoJ MansM ReveringR RusackR SaradhyN SchroederN StrobbeM A WadudJ G AcostaS OliverosK BloomS ChauhanD R ClaesC FangmeierL FincoF GolfJ R González FernándezI KravchenkoJ E SiadoG R SnowB StiegerW TabbF YanG AgarwalH BandyopadhyayC HarringtonL HayI IashviliA KharchilavaC McLeanD NguyenJ PekkanenS RappoccioB RoozbahaniCms CollaborationE BarberisC FreerY HaddadA HortiangthamJ LiG MadiganB MarzocchiD M MorseV NguyenT OrimotoA ParkerL SkinnariA Tishelman-CharnyT WamorkarB WangA WisecarverD WoodS BhattacharyaJ BueghlyZ ChenA GilbertT GunterK A HahnN OdellM H SchmittK SungM VelascoR BucciN DevR GoldouzianM HildrethK Hurtado AnampaC JessopD J KarmgardK LannonW LiN LoukasN MarinelliI McalisterF MengK MohrmanY MusienkoR RuchtiP SiddireddyS TaroniM WayneA WightmanM WolfL ZygalaJ AlimenaB BylsmaB CardwellL S DurkinB FrancisC HillA LefeldB L WinerB R YatesP DasG DezoortP ElmerB GreenbergN HaubrichS HigginbothamA KalogeropoulosG KoppS KwanD LangeM T LucchiniJ LuoD MarlowK MeiI OjalvoJ OlsenC PalmerP PirouéD SticklandC TullySudhir MalikS NorbergV E BarnesR ChawlaS DasL GutayM JonesA W JungB MahakudG NegroN NeumeisterC C PengS PiperovH QiuJ F SchulteM StojanovicN TrevisaniF WangR XiaoW XieT ChengJ DolenN ParasharA BatyS DildickK M EcklundS FreedF J M GeurtsM KilpatrickA KumarW LiB P PadleyR RedjimiJ RobertsJ RorieW ShiA G Stahl LeitonA BodekP de BarbaroR DeminaJ L DulembaC FallonT FerbelM GalantiA Garcia-BellidoO HindrichsA KhukhunaishviliE RankenR TausB ChiaritoJ P ChouA GandrakotaY GershteinE HalkiadakisA HartM HeindlE HughesS KaplanO KarachebanI LaflotteA LathR MontalvoK NashM OshersonS SalurS SchnetzerS SomalwarR StoneS A ThayilS ThomasH WangH AcharyaA G DelannoyS SpanierOthmane BouhaliM DalchenkoA DelgadoR EusebiJ GilmoreT HuangT KamonH KimS LuoS MalhotraR MuellerD OvertonL PernièD RathjensA SafonovJ SturdyN AkchurinJ DamgovV HegdeS KunoriK LamichhaneS W LeeT MengkeS MuthumuniT PeltolaS UndleebI VolobouevZ WangA WhitbeckE AppeltS GreeneA GurrolaR JanjamW JohnsC MaguireA MeloH NiK PadekenF RomeoP SheldonS TuoJ VelkovskaM VerweijM W ArentonB CoxG CummingsJ HakalaR HiroskyM JoyceA LedovskoyA LiC NeuB TannenwaldY WangE WolfeF XiaP E KarchinN PoudyalP ThapaK BlackT BoseJ BuchananC CaillolS DasuI De BruynP EveraertsC GalloniH HeM HerndonA HervéU HussainA LanaroA LoeligerR LovelessJ Madhusudanan SreekalaA MallampalliD PinnaT RugglesA SavinV ShangV SharmaW H SmithD TeagueS Trembath-ReichertW Vetensnull nullPublished in: The European physical journal. C, Particles and fields (2021)
A search is presented for supersymmetric partners of the top quark (top squarks) in final states with two oppositely charged leptons (electrons or muons), jets identified as originating from b quarks, and missing transverse momentum. The search uses data from proton-proton collisions at s = 13 TeV collected with the CMS detector, corresponding to an integrated luminosity of 137 fb - 1 . Hypothetical signal events are efficiently separated from the dominant top quark pair production background with requirements on the significance of the missing transverse momentum and on transverse mass variables. No significant deviation is observed from the expected background. Exclusion limits are set in the context of simplified supersymmetric models with pair-produced lightest top squarks. For top squarks decaying exclusively to a top quark and a lightest neutralino, lower limits are placed at 95 % confidence level on the masses of the top squark and the neutralino up to 925 and 450 GeV , respectively. If the decay proceeds via an intermediate chargino, the corresponding lower limits on the mass of the lightest top squark are set up to 850 GeV for neutralino masses below 420 GeV . For top squarks undergoing a cascade decay through charginos and sleptons, the mass limits reach up to 1.4 TeV and 900 GeV respectively for the top squark and the lightest neutralino.