6533b852fe1ef96bd12aab3f

RESEARCH PRODUCT

Measurement of the top quark mass andpp¯→tt¯cross section in the all-hadronic mode with the CDF II detector

K. GibsonE. PalenciaStanislav TokárAdrian BuzatuM. CampbellM. CampbellP. GirominiC. P. MarinoJ. L. GimmellMichael L. NormanJulia ThomJulia ThomG. A. ThompsonIvan-kresimir FuricG. VelevA. GreseleF. SforzaF. SforzaS. Z. ShalhoutV. MartinD. O. LitvintsevBernd StelzerA. MenzioneC. S. MoonB. CarlsN. KrumnackN. MoggiS. De CeccoA. SimonenkoM. RossiJ. E. KimC. FerrazzaS. DubeA. RuizF. VázquezF. VázquezS. NeubauerS. Y. TsaiS. RolliG. MitselmakherF. HappacherPavol BartosC. HaberDean HidasJ. Guimaraes Da CostaO. PoukhovA. ElaginA. T. LaasanenJ. C. FreemanH. GerberichC. MesropianV. RusuV. CavaliereR. MooreS. C. HsuR. L. WagnerY. C. ChenM. LancasterH. WolfeJ. GalyardtAndrew IvanovAndrew IvanovKevin LannonKevin LannonM. E. MattsonD. CauzD. CauzD. HirschbuehlD. GlenzinskiM. J. FrankAnna SfyrlaN. RanjanStefano ZucchelliR. EusebiT. LiuAndrew BeretvasG. IntrozziY. TuN. S. LockyerD. WatersDaniela BortolettoP. E. KarchinD. H. KimKyeongjae ChoSatoru UozumiS. FarringtonJ. PursleyPaola GiannettiB. A. BarnettS. JindarianiGiorgio ApollinariV. RamakrishnanF. ProkoshinF. ProkoshinGuillelmo Gomez-ceballosJ. AntosJ. AntosJ. Wagner-kuhrMichele GallinaroPeter WittichPeter WittichC. MarinoJ. WeineltA. LathH. MiyakeC. PagliaroneKai YiKai YiMark NeubauerI. LazzizzeraJ. P. FernandezG. ChiarelliS. GrinsteinA. PapaikonomouTeruki KamonL. PondromMichael SchmittW. H. ChungT. J. PhillipsM. LindgrenI. SuslovA. MartinA. MartinM. E. ConveryS. H. KimF. CanelliAlberto AnnoviY. SeiyaB. KilminsterM. DeninnoD. W. GerdesLuca ScodellaroP. De BarbaroVirgil E BarnesCraig BlockerJ. ConwayM. StanitzkiA. A. ParamanovAidan RobsonD. P. BenjaminY. KatoY. KatoJ. E. JungA. Di CantoP. F. ShepardD. E. PellettA. N. SisakyanD. ErredeC. M. GinsburgW. BadgettJ. A. AppelJiawei HanP. H. BeaucheminS. TkaczykGiovanni BellettiniV. SorinRainer WallnyK. L. ByrumT. MiaoD. ChokheliJ. P. ChouM. CordelliBrian L WinerJ. HeuserIvan VilaR. G. WagnerFrank WürthweinL. E. KirschD. AmideiP. MuratAndrea BocciJ. MorlockR. VilarG. ChlachidzeKoji SatoM. PauliniAnna ZanettiP. MazzantiR. ForrestJ. PatrickPetar MaksimovicThorsten ChwalekL. RistoriE. LeeE. LeeB. RutherfordN. Van RemortelN. Van RemortelJoe IncandelaJ. E. GarciaC. PlagerXin WuF. GarbersonMauro Dell'orsoS. R. HouFrancesco CrescioliC. BrombergD. W. JangAlessandro CerriM. ShimojimaM. ShimojimaJ. S. SuhMatteo Cavalli-sforzaA. T. GoshawA. PenzoT. LecompteM. A. SchmidtN. D'ascenzoHye-sung LeeFranco BedeschiW. T. FedorkoSally SeidelSang Woon LeeM. GoncharovM. GoncharovY. C. YangH. C. FangJ. LueckJ. NaganomaR. St. DenisAndreas WarburtonS. S. YuAvraham YagilE. ThomsonManuela CampanelliY. ZengK. EbinaM. WeinbergerM. MartínezR. E. HughesM. D'erricoD. TonelliEva HalkiadakisM. N. MondragonM. N. MondragonT. WrightE. RogersP. GarosiP. GarosiC. WolfeI. ShreyberD. KropG. P. YehC. Grosso-pilcherV. A. GiakoumopoulouR. F. HarrTara ShearsM. K. JhaA. BridgemanE. WicklundS. DonatiT. AaltonenT. DorigoAnyes TaffardAnyes TaffardP. MehtalaC. Cuenca AlmenarM. J. KimS. LamiA. BodekY. ZhengY. ZhengB. CasalJ. LinacreJ. C. YunJ. MülmenstädtChris HaysE. LipelesV. KhotilovichS. CarronJ. R. DittmannR. Martínez-ballarínG. WilliamsM. A. HouldenA. RahamanK. PotamianosJian TangH. S. BuddR. LysakA. AurisanoJ. SlaunwhiteAntonio BoveiaM. HartzJ. AsaadiJ. N. BellingerM. KurataK. MakhoulD. KarA. G. ClarkA. B. WicklundP. BarriaM. CorboP. RentonE. JamesJ. C. CullyFabrizio MargaroliM. MathisAron SohaS. R. HahnMarcelo VogelJavier CuevasJavier CuevasX. ZhangN. KimuraL. PineraS. BehariY. K. KimJ. BoudreauR. KephartJ. DengT. WakisakaT. WakisakaK. MaeshimaAndrea CastroC. I. CiobanuR. MadrakL. SantiJ. S. LeeS. CarrilloTomoko YoshidaTomoko YoshidaM. J. ShochetW. KetchumR. E. BlairA. SchmidtG. CompostellaMaria Agnese CiocciL. Sexton-kennedyN. P. KulkarniS. RichterJ. YohK. GoulianosM. HeckA. HockerM. FranklinL. OakesJane NachtmanM. MilnikE. PueschelJ. NettP. WilsonB. JayatilakaE. VatagaRichard D FieldC. VellidisA. GolossanovMark KruseAlison ListerJ. BudagovPaul TiptonV. PapadimitriouJonas RademackerJonas RademackerC. DelucaAndrew MehtaB. WhitehouseS. Y. JunK. KondoG. PunziG. VolpiGervasio GomezP. MastrandreaG. GiurgiuM. J. MorelloIgnacio RedondoF. PtohosF. PtohosB. ÁLvarez GonzálezB. ÁLvarez GonzálezJason NielsenJason NielsenD. J. KongTh. MüllerG. LunguN. ErshaidatN. ErshaidatR. RoserKoji YamamotoY. ShonK. HatakeyamaL. SartoriAlexei SafonovP. K. TengK. SliwaB. BrauB. BrauP. Ttito-guzmánW. AshmanskasSudhir MalikM. VidalS. KlimenkoS. MoedJ. StrologasM. HusseinY. S. ChungMonica D'onofrioE. PianoriK. NakamuraN. GiokarisSong-ming WangJ. HeinrichF. AzfarM. TrovatoIntae YuM. RescignoT. R. JunkA. NapierS. HewamanageKazuhiko HaraRobin ErbacherM. DattaW-m. YaoA. AnastassovK. S. McfarlandA. KorytovN. MiladinovicJ. YamaokaI. OksuzianA. Savoy-navarroA. AttalA. J. SlaughterR. TakashimaK. BurkettO. Stelzer-chiltonShih-hsin ChangVyacheslav KrutelyovD. BeecherPeter WagnerM. MussiniO. GonzálezS. PashapourM. BinkleyV. BoisvertG. De LorenzoJ. HustonA. MitraP. DongD. LucchesiA. ApresyanZ. Gunay-unalanP. J. BusseyA. Manousakis-katsikakisStefano CamardaS. CabreraF. ChlebanaEmily NurseM. GiuntaM. IoriR. McnultyR. McnultyM. TecchioW. JohnsonA. VarganovV. GlagolevFabrizio ScuriDuncan CarlsmithFumihiko UkegawaT. SchwarzE. E. SchmidtD. DagenhartH. H. WilliamsL. LovasDaniel WhitesonDaniel WhitesonT. PeifferB. Y. HanJ. KrollU. K. YangU. K. YangR. CarosiK. TollefsonC. MillsDario BiselloS. ErredeA. BhattiM. KrepsIgor VolobouevIgor VolobouevP. SchlabachY. D. OhG. LatinoA. ArtikovU. GrundlerH. S. KimG. L. StryckerT. KuhrA. LoginovR. L. LanderJames RussBarry BlumenfeldN. GoldschmidtS. MaldeJ. ThomeE. J. JeonF. RimondiU. HusemannS. B. KimA. CanepaS. BuddY. TakeuchiK. K. JooS. ShiraishiD. MietlickiR. RossinS. KwangV. SavelievD. TobackA. MukherjeeA. V. KotwalJ. KonigsbergK. ChungI. GorelovW. C. WesterS. H. OhE. BrubakerReisaburo TanakaItsuo NakanoAlan GarfinkelP. McintyreT. DaviesM. HurwitzKohei YoritaC. S. HillC. S. HillSandra LeoneW. K. SakumotoP. RoyT. RodriguezC. J. LinM. GoldA. PronkoRobert SnihurG. PaulettaN. TuriniD. StentzD. TorrettaA. SemenovB. ParksD. ClarkWolfgang WagnerScott WilburS. AmerioS. SomalwarD. MacqueenM. HerndonL. BrigliadoriP. LukensJahred AdelmanL. NodulmanG. BauerF. D. SniderP. LujanS. WolbersStephan LammelLucio CerritoLucio CerritoYoshikazu NagaiA. SukhanovT. TomuraS. Pagan GrisoG. PiacentinoJ. D. LewisT. RodrigoP. Movilla FernandezHeimo SaarikkoA. SedovM. RenzJ. KeungT. OkusawaJ. R. SmithG. B. YuR. MillerJ. LysM. GiordaniC.t. LiuChristoph PausS. GiaguS. GiaguD. J. CoxM. FeindtM. JonesB. Di RuzzaA. ScribanoS. TorreG. FlanaganP. TotaroMaxwell ChertokH. W. KimI. BizjakI. BizjakA. GesslerP. SinervoA. Barbaro-galtieriG. BusettoP. SquillaciotiP. SquillaciotiG. MancaK. OsterbergK. PittsM. P. SchmidtR. OravaL. DemortierP. CatastiniA. DeisherMassimo CasarsaM. HareC. CalanchaD. HareR. CulbertsonO. NorniellaC. A. CoxR. G. FeildTetsuo ArisawaC. Neu

subject

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsTop quarkMass distribution010308 nuclear & particles physicsHadronTevatron01 natural sciencesBottom quarkNuclear physicsPair production0103 physical sciencesMass spectrumHigh Energy Physics::Experiment010306 general physics

description

We present a measurement of the top quark mass and of the top-antitop pair production cross section using p-pbar data collected with the CDFII detector at the Tevatron Collider at the Fermi National Accelerator Laboratory and corresponding to an integrated luminosity of 2.9 fb-1. We select events with six or more jets satisfying a number of kinematical requirements imposed by means of a neural network algorithm. At least one of these jets must originate from a b quark, as identified by the reconstruction of a secondary vertex inside the jet. The mass measurement is based on a likelihood fit incorporating reconstructed mass distributions representative of signal and background, where the absolute jet energy scale (JES) is measured simultaneously with the top quark mass. The measurement yields a value of 174.8 +- 2.4(stat+JES) ^{+1.2}_{-1.0}(syst) GeV/c^2, where the uncertainty from the absolute jet energy scale is evaluated together with the statistical uncertainty. The procedure measures also the amount of signal from which we derive a cross section, sigma_{ttbar} = 7.2 +- 0.5(stat) +- 1.0 (syst) +- 0.4 (lum) pb, for the measured values of top quark mass and JES.

https://doi.org/10.1103/physrevd.81.052011