6533b828fe1ef96bd12881b9
RESEARCH PRODUCT
Precision Measurement of the Top Quark Mass in <span class="aps-inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><mstyle mathvariant="normal"><mi>L</mi></mstyle><mtext mathvariant="bold">epton</mtext><mo>+</mo><mstyle mathvariant="normal"><mi>J</mi></mstyle><mtext mathvariant="bold">ets</mtext></mrow></math></span> Final States
L. S. VertogradovG. W. WilsonChristopher George TullyThibault GuilleminU. BasslerA. DasP. SvoiskyJ. KrausRegina DeminaPatrick SlatteryClaus P. BuszelloEmily JohnsonHui LiA. S. ItoA. JayasingheY. A. YatsunenkoMarkus WobischMaxim PerfilovI. Ripp-baudotA. MeyerS. CihangirS. ChakrabartiY. T. TsaiFabrice CoudercY. IlchenkoJ. OrdunaP. RubinovM. EadsM. JaffréLiang LiAlexander KupcoI. KatsanosR. D. SchambergerN. ParuaD. VilanovaRandy RuchtiE. De La Cruz-bureloM. C. CousinouCarlos AvilaJ. ZennamoA. DubeyF. BadaudLev DudkoZdenek HubacekJose Andres Garcia-gonzalezJ. M. HauptmanCecilia Elena GerberR. BernhardW. E. CooperG. GintherG. GintherM. P. SandersVladimir GavrilovJi ZhuW. M. Van LeeuwenRobert HiroskyJoseph HaleyGordon WattsJ. ClutterPhillip GutierrezAndrew BrandtJ. WeichertJianming QianS. DesaiCecile DeterreP. NeustroevPetr VokacChristophe RoyonD. MenezesY. W. LiuL. Welty-riegerS. AtkinsW. M. LeeR. Van KootenW. GengW. GengR. IllingworthCarsten HenselG. GutierrezHongfang LiuA. MelnitchoukArnaud DuperrinGuennadi BorissovI. Heredia-de La CruzSuneel DuttM. D. CorcoranH. D. WahlS. BhatiaV. V. LipaevJ. LellouchW. C. FisherN. K. MondalD. BolineN. KhalatyanUlrich HeintzMarco VerzocchiM. H.l.s. WangF. MiconiPedro G MercadanteXiaowen LeiDon LincolnErich VarnesH. T. DiehlD. SmirnovA. BoehnleinV. E. BazterraL. HanK. DevaughanAndreas Werner JungOleg BrandtJ. P. AgnewA. PatwaG. D. AlexeevFlera RizatdinovaL. FengA. AltonPhilip BaringerK. HernerNeeti ParasharJ. HoganJ. EllisonS. FuessMarcia BegalliJ. SnowShangfeng YangL. BellantoniMarc BesanconT. KurcaT. KurcaJ. Martínez-ortegaI. RazumovS. BanerjeeH. E. FiskM. ZielinskiSung Keun ParkBjoern PenningMeenakshi NarainJ. HaysD. HedinYuji EnariFrank FilthautSuyong ChoiSteven W. ShawShih-chang LeeM. DiesburgEmilien ChaponM. SavitskyiElizaveta ShabalinaJ. WarcholA. FauréNikos VarelasC. L. McgivernBing ZhouAnthony RossV. M. AbazovA. Y. VerkheevM. M. MeijerK. A. JohnsAran Garcia-bellidoY. N. KharzheevAlexander GrohsjeanX. B. BuG. GolovanovEmanuela BarberisHang YinM. VesterinenLev UvarovP. N. RatoffY. PetersT. YasudaD. EdmundsAaron DominguezMaksym TitovD. V. BandurinJean-arcady MeyerS. GrederA. JonckheereD. KarmanovS. J. De JongAngelo De Souza SantosL. BagbyIain Alexander BertramR. MadarA. LobodenkoE. E. BoosMartin GrunewaldZhenyu YeKamil AugstenM. CookeGregorio BernardiD. DenisovD. A. StoyanovaYuri GershteinHeriberto Castilla-valdezLidija ZivkovicSergey BurdinK. M. ChanA. A. ShchukinT. G. ZhaoW. YeAshok KumarFrank FiedlerS. P. DenisovDaria ZieminskaHal EvansThomas FerbelMilos LokajicekP. D. GrannisM. BorysovaE. Camacho-pérezD. LiE. KajfaszV. N. EvdokimovM. PrewittLars SonnenscheinD. N. BrownM. RominskyH. HegabV. PariharSudhir MalikIa IashviliReinhard SchwienhorstDmitri TsybychevR. L. MccarthyT. R. WyattB. C.k. CaseyJ. L. HolzbauerJ. SekaricMichael A. StraussM. HohlfeldBrajesh C ChoudharyMichael MulhearnV. BunichevMark Richard James WilliamsV. V. SharyJ. P. NegretDarien WoodR. Luna-garciaPushpalatha C BhatJ. JoshiMichael HildrethAvto KharchilavaA. K.a. MacielO. GogotaDarren PriceR. JesikMarvin JohnsonB. HoeneisenH. T. NguyenT. HoangLee SawyerS. UzunyanAlexander KhanovH. GreenleeA. L. LyonA. V. KozelovB. S. AcharyaS. Söldner-remboldS. BlessingAmnon HarelA. BrossT. ScanlonGuo-ming ChenS. KermicheN. ProkopenkoJ. F. BartlettRobert KehoeP. F. DingScott SnyderSuman Bala BeriV. HynekS. W. YounJohn HobbsRuchika NayyarJ. M. YuJ. K. LimA. V. PopovM. R. AdamsT. HeadG. GrenierG. GrenierA. P. HeinsonD. R. ClaesT. NunnemannBrad AbbottM. A. PleierB. BaldinV. V. TokmeninG. AlkhazovTodd AdamsGavin DaviesV. M. PodstavkovR. Lopes De SaPierre PetroffH. A. NealJ. T. LinnemannGregory R SnowK. YipJason Dhia MansourM. FortnerA. ChandraY. ScheglovPh GrisP. LebrunP. LebrunJan StarkVictor Daniel ElviraP. H. GarbinciusA. Sanchez-hernandezAndrew AskewV. SimakSabine LammersV. A. KuzminMitchell WayneH. SchellmanJ. M. KohliStefan GrünendahlM. BuehlerB. TuchmingP. SkubicR. Magaña-villalbaS. W. ChoGianluca PetrilloShabnam JabeenM. MerkinI. HowleyRaymond BrockR. BeuselinckG. C. BlazeyS. CaughronArnulf QuadtY. XieElemer NagyN. OsmanP. JiangFrederic DeliotG. SavageR. YamadaJean-francois GrivazP. JonssonA. PalThomas HebbekerQ. Z. LiI. KiselevichA. JusteK. PetridisHarald FoxKristian HarderJ. OstaL. SuterD. CuttsI. A. VasilyevK. SoustruznikG. SajotHorst SeveriniHakjae LeeRichard B. LiptonS. UvarovB. QuinnC. SchwanenbergerAlice BeanVolker BuescherVipin BhatnagarR. PartridgeKenneth BloomV. L. MalyshevM. S. JeongGavin Grant Heskethsubject
PhysicsTop quarkParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomyD0 experiment7. Clean energylaw.inventionNuclear physicslawHigh Energy Physics::ExperimentProduction (computer science)FermilabColliderBosonLeptondescription
We measure the mass of the top quark in lepton$+$jets final states using the full sample of $$p\bar{p}$$ collision data collected by the D0 experiment in Run II of the Fermilab Tevatron Collider at $$\sqrt s=1.96 $$TeV, corresponding to $$9.7 {\rm fb}^{-1}$$ of integrated luminosity. We use a matrix element technique that calculates the probabilities for each event to result from $$t\bar t$$ production or background. The overall jet energy scale is constrained in situ by the mass of the $W$ boson. We measure $$m_t=174.98\pm0.76$$ GeV. In conclusion, this constitutes the most precise single measurement of the top-quark mass.
year | journal | country | edition | language |
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2014-07-17 | Physical Review Letters |