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We present a measurement of the mass of the top quark using data corresponding to an integrated luminosity of 1.9fb^-1 of ppbar collisions collected at sqrt{s}=1.96 TeV with the CDF II detector at Fermilab's Tevatron. This is the first…

High Energy Physics - Experiment · Physics 2010-05-12 CDF Collaboration , T. Aaltonen

We present a measurement of the top-quark mass using a sample of $t\bar{t}$ events in 5.7 fb$^{-1}$ of integrated luminosity from $p\bar{p}$ collisions at the Fermilab Tevatron with $\sqrt{s} =$ 1.96 TeV and collected by the CDF II…

High Energy Physics - Experiment · Physics 2014-08-28 CDF Collaboration

The mass of the top quark is measured using a sample of t t-bar candidate events with one electron or muon and at least four jets in the final state, collected by CMS in pp collisions at sqrt(s) = 7 TeV at the LHC. A total of 5174 candidate…

High Energy Physics - Experiment · Physics 2013-03-19 The CMS Collaboration

A top quark mass measurement is performed using 35.9 fb$^{-1}$ of LHC proton-proton collision data collected with the CMS detector at $\sqrt{s} =$ 13 TeV. The measurement uses the $\mathrm{t\overline{t}}$ all-jets final state. A kinematic…

High Energy Physics - Experiment · Physics 2019-04-09 CMS Collaboration

The most precise measurements of the top quark mass are based on the Matrix Element method. We present a detailed description of this analysis method, taking the measurements of the top quark mass in final states with one and two charged…

High Energy Physics - Experiment · Physics 2011-03-28 Frank Fiedler , Alexander Grohsjean , Petra Haefner , Philipp Schieferdecker

We report on recent measurements of the top quark mass using t t-bar candidate events selected in ~320/pb of data from the "Run II" operation period of the Tevatron p p-bar collider. More emphasis is given on the best single measurement to…

High Energy Physics - Experiment · Physics 2007-05-23 Kostas Kordas

A measurement of the top-quark mass is presented using Tevatron data from proton-antiproton collisions at center-of-mass energy $\sqrt{s}=1.96$ TeV collected with the CDF II detector. Events are selected from a sample of candidates for…

High Energy Physics - Experiment · Physics 2011-10-17 CDF Collaboration , T. Aaltonen , B. Álvarez Gonzálezv , S. Amerio , D. Amidei , A. Anastassov , A. Annovi , J. Antos , G. Apollinari , J. A. Appel , A. Apresyan , T. Arisawa , A. Artikov , J. Asaadi , W. Ashmanskas , B. Auerbach , A. Aurisano , F. Azfar , W. Badgett , A. Barbaro-Galtieri , V. E. Barnes , B. A. Barnett , P. Barriaee , P. Bartos , M. Baucecc , G. Bauer , F. Bedeschi , D. Beecher , S. Behari , G. Bellettinidd , J. Bellinger , D. Benjamin , A. Beretvas , A. Bhatti , M. Binkley , D. Bisellocc , I. Bizjakii , K. R. Bland , C. Blocker , B. Blumenfeld , A. Bocci , A. Bodek , D. Bortoletto , J. Boudreau , A. Boveia , B. Braua , L. Brigliadoribb , A. Brisuda , C. Bromberg , E. Brucken , M. Bucciantoniodd , J. Budagov , H. S. Budd , S. Budd , K. Burkett , G. Busettocc , P. Bussey , A. Buzatu , S. Cabrerax , C. Calancha , S. Camarda , M. Campanelli , M. Campbell , F. Canelli , A. Canepa , B. Carls , D. Carlsmith , R. Carosi , S. Carrillok , S. Carron , B. Casal , M. Casarsa , A. Castrobb , P. Catastini , D. Cauz , V. Cavaliereee , M. Cavalli-Sforza , A. Cerrif , L. Cerritoq , Y. C. Chen , M. Chertok , G. Chiarelli , G. Chlachidze , F. Chlebana , K. Cho , D. Chokheli , J. P. Chou , W. H. Chung , Y. S. Chung , C. I. Ciobanu , M. A. Ciocciee , A. Clark , D. Clark , G. Compostellacc , M. E. Convery , J. Conway , M. Corbo , M. Cordelli , C. A. Cox , D. J. Cox , F. Cresciolidd , C. Cuenca Almenar , J. Cuevasv , R. Culbertson , D. Dagenhart , N. d'Ascenzot , M. Datta , P. de Barbaro , S. De Cecco , G. De Lorenzo , M. Dell'Orsodd , C. Deluca , L. Demortier , J. Dengc , M. Deninno , F. Devoto , M. d'Erricocc , A. Di Cantodd , B. Di Ruzza , J. R. Dittmann , M. D'Onofrio , S. Donatidd , P. Dong , T. Dorigo , K. Ebina , A. Elagin , A. Eppig , R. Erbacher , D. Errede , S. Errede , N. Ershaidataa , R. Eusebi , H. C. Fang , S. Farrington , M. Feindt , J. P. Fernandez , C. Ferrazzaff , R. Field , G. Flanaganr , R. Forrest , M. J. Frank , M. Franklin , J. C. Freeman , I. Furic , M. Gallinaro , J. Galyardt , J. E. Garcia , A. F. Garfinkel , P. Garosiee , H. Gerberich , E. Gerchtein , S. Giagugg , V. Giakoumopoulou , P. Giannetti , K. Gibson , C. M. Ginsburg , N. Giokaris , P. Giromini , M. Giunta , G. Giurgiu , V. Glagolev , D. Glenzinski , M. Gold , D. Goldin , N. Goldschmidt , A. Golossanov , G. Gomez , G. Gomez-Ceballos , M. Goncharov , O. González , I. Gorelov , A. T. Goshaw , K. Goulianos , A. Gresele , S. Grinstein , C. Grosso-Pilcher , R. C. Group , J. Guimaraes da Costa , Z. Gunay-Unalan , C. Haber , S. R. Hahn , E. Halkiadakis , A. Hamaguchi , J. Y. Han , F. Happacher , K. Hara , D. Hare , M. Hare , R. F. Harr , K. Hatakeyama , C. Hays , M. Heck , J. Heinrich , M. Herndon , S. Hewamanage , D. Hidas , A. Hocker , W. Hopkinsg , D. Horn , S. Hou , R. E. Hughes , M. Hurwitz , U. Husemann , N. Hussain , M. Hussein , J. Huston , G. Introzzi , M. Iorigg , A. Ivanovo , E. James , D. Jang , B. Jayatilaka , E. J. Jeon , M. K. Jha , S. Jindariani , W. Johnson , M. Jones , K. K. Joo , S. Y. Jun , T. R. Junk , T. Kamon , P. E. Karchin , Y. Katon , W. Ketchum , J. Keung , V. Khotilovich , B. Kilminster , D. H. Kim , H. S. Kim , H. W. Kim , J. E. Kim , M. J. Kim , S. B. Kim , S. H. Kim , Y. K. Kim , N. Kimura , S. Klimenko , K. Kondo , D. J. Kong , J. Konigsberg , A. Korytov , A. V. Kotwal , M. Kreps , J. Kroll , D. Krop , N. Krumnackl , M. Kruse , V. Krutelyovd , T. Kuhr , M. Kurata , S. Kwang , A. T. Laasanen , S. Lami , S. Lammel , M. Lancaster , R. L. Lander , K. Lannonu , A. Lath , G. Latinoee , I. Lazzizzera , T. LeCompte , E. Lee , H. S. Lee , J. S. Lee , S. W. Leew , S. Leodd , S. Leone , J. D. Lewis , C. -J. Lin , J. Linacre , M. Lindgren , E. Lipeles , A. Lister , D. O. Litvintsev , C. Liu , Q. Liu , T. Liu , S. Lockwitz , N. S. Lockyer , A. Loginov , D. Lucchesicc , J. Lueck , P. Lujan , P. Lukens , G. Lungu , J. Lys , R. Lysak , R. Madrak , K. Maeshima , K. Makhoul , P. Maksimovic , S. Malik , G. Mancab , A. Manousakis-Katsikakis , F. Margaroli , C. Marino , M. Martínez , R. Martínez-Ballarín , P. Mastrandrea , M. Mathis , M. E. Mattson , P. Mazzanti , K. S. McFarland , P. McIntyre , R. McNultyi , A. Mehta , P. Mehtala , A. Menzione , C. Mesropian , T. Miao , D. Mietlicki , A. Mitra , H. Miyake , S. Moed , N. Moggi , M. N. Mondragonk , C. S. Moon , R. Moore , M. J. Morello , J. Morlock , P. Movilla Fernandez , A. Mukherjee , Th. Muller , P. Murat , M. Mussinibb , J. Nachtmanm , Y. Nagai , J. Naganoma , I. Nakano , A. Napier , J. Nett , C. Neuz , M. S. Neubauer , J. Nielsene , L. Nodulman , O. Norniella , E. Nurse , L. Oakes , S. H. Oh , Y. D. Oh , I. Oksuzian , T. Okusawa , R. Orava , L. Ortolan , S. Pagan Grisocc , C. Pagliarone , E. Palenciaf , V. Papadimitriou , A. A. Paramonov , J. Patrick , G. Paulettahh , M. Paulini , C. Paus , D. E. Pellett , A. Penzo , T. J. Phillips , G. Piacentino , E. Pianori , J. Pilot , K. Pitts , C. Plager , L. Pondrom , K. Potamianos , O. Poukhov , F. Prokoshiny , A. Pronko , F. Ptohosh , E. Pueschel , G. Punzidd , J. Pursley , A. Rahaman , V. Ramakrishnan , N. Ranjan , I. Redondo , P. Renton , M. Rescigno , F. Rimondibb , L. Ristori , A. Robson , T. Rodrigo , T. Rodriguez , E. Rogers , S. Rolli , R. Roser , M. Rossi , F. Ruffiniee , A. Ruiz , J. Russ , V. Rusu , A. Safonov , W. K. Sakumoto , L. Santihh , L. Sartori , K. Sato , V. Savelievt , A. Savoy-Navarro , P. Schlabach , A. Schmidt , E. E. Schmidt , M. P. Schmidt , M. Schmitt , T. Schwarz , L. Scodellaro , A. Scribanoee , F. Scuri , A. Sedov , S. Seidel , Y. Seiya , A. Semenov , F. Sforzadd , A. Sfyrla , S. Z. Shalhout , T. Shears , P. F. Shepard , M. Shimojimas , S. Shiraishi , M. Shochet , I. Shreyber , A. Simonenko , P. Sinervo , A. Sissakian , K. Sliwa , J. R. Smith , F. D. Snider , A. Soha , S. Somalwar , V. Sorin , P. Squillacioti , M. Stanitzki , R. St. Denis , B. Stelzer , O. Stelzer-Chilton , D. Stentz , J. Strologas , G. L. Strycker , Y. Sudo , A. Sukhanov , I. Suslov , K. Takemasa , Y. Takeuchi , J. Tang , M. Tecchio , P. K. Teng , J. Thomg , J. Thome , G. A. Thompson , E. Thomson , P. Ttito-Guzmán , S. Tkaczyk , D. Toback , S. Tokar , K. Tollefson , T. Tomura , D. Tonelli , S. Torre , D. Torretta , P. Totarohh , M. Trovatoff , Y. Tu , N. Turiniee , F. Ukegawa , S. Uozumi , A. Varganov , E. Vatagaff , F. Vázquez , G. Velev , C. Vellidis , M. Vidal , I. Vila , R. Vilar , M. Vogel , G. Volpidd , P. Wagner , R. L. Wagner , T. Wakisaka , R. Wallny , S. M. Wang , A. Warburton , D. Waters , M. Weinberger , W. C. Wester , B. Whitehouse , D. Whitesonc , A. B. Wicklund , E. Wicklund , S. Wilbur , F. Wick , H. H. Williams , J. S. Wilson , P. Wilson , B. L. Winer , P. Wittichg , S. Wolbers , H. Wolfe , T. Wright , X. Wu , Z. Wu , K. Yamamoto , J. Yamaoka , T. Yang , U. K. Yangp , Y. C. Yang , W. -M. Yao , G. P. Yeh , K. Yim , J. Yoh , K. Yorita , T. Yoshidaj , G. B. Yu , I. Yu , S. S. Yu , J. C. Yun , A. Zanetti , Y. Zeng , S. Zucchelli

A first measurement of the top quark mass using the decay channel t to (W to l nu) (b to J/psi + X to mu+ mu- + X) is presented. The analysis uses events selected from the proton-proton collisions recorded with the CMS detector at the LHC…

High Energy Physics - Experiment · Physics 2017-01-02 CMS Collaboration

We present a measurement of the mass of the top quark from ppbar collisions at 1.96 TeV observed with the Collider Detector at Fermilab (CDF) at the Fermilab Tevatron Run II. The events have the decay signature of ppbar to ttbar in the…

High Energy Physics - Experiment · Physics 2007-05-23 Brian Mohr

We present a new measurement of the mass of the top quark using lepton + jets ttbar events collected by the DO experiment in Run I of the Fermilab Tevatron Collider. The mass is extracted through a comparison of each event with a…

High Energy Physics - Experiment · Physics 2007-05-23 V. M. Abazov , The D0 Collaboration

The CDF and D0 collaborations have updated their measurements of the mass of the top quark using proton-antiproton collisions at sqrt{s}=1.96TeV produced at the Tevatron. The uncertainties in each of the of top-antitop decay channels have…

High Energy Physics - Experiment · Physics 2019-08-14 Pedro A. Movilla Fernandez

This article presents a measurement of the top quark mass using the CDF II detector at Fermilab. Colliding beams of protons and anti-protons at Fermilab's Tevatron (sqrt{s}=1.96 TeV) produce top/anti-top pairs, which decay to W^+W^-bbbar;…

High Energy Physics - Experiment · Physics 2012-08-27 CDF Collaboration

The latest measurements of the top quark mass obtained by the ATLAS and CMS experiments at the LHC for centre-of-mass energies of 7 and 8 TeV are presented. The mass of the top quark is measured using several methods and channels, including…

High Energy Physics - Experiment · Physics 2015-09-11 Sven Menke

We consider photon radiation in tbar-t events at the upgraded Fermilab Tevatron and the CERN Large Hadron Collider (LHC) as a tool to measure the electric charge of the top quark. We analyze the contributions of tbar-t-gamma production and…

High Energy Physics - Phenomenology · Physics 2009-11-07 U. Baur , M. Buice , L. H. Orr

We describe a measurement of the top quark mass using events with two charged leptons collected by the CDF II detector from $p\bar{p}$ collisions with $\sqrt s = 1.96$ TeV at the Fermilab Tevatron. The likelihood in top mass is calculated…

High Energy Physics - Experiment · Physics 2010-05-12 A. Abulencia

I give an overview of recent results on top quark properties and interactions, obtained using data collected with the CMS experiment during the years 2010--2011 at sqrt(s)= 7 TeV. Measurements are presented for the inclusive top pair…

High Energy Physics - Experiment · Physics 2019-08-13 Karl M. Ecklund

The top quark mass is measured in the $t\bar{t}\to$ dilepton channel (lepton $= e, \mu$) using ATLAS data recorded in the year 2012 at the LHC. The data were taken at a proton--proton centre-of-mass energy of $\sqrt{s}=$ 8 TeV and…

High Energy Physics - Experiment · Physics 2016-09-22 ATLAS Collaboration

We propose a new method to measure various physical parameters, using characteristic weight functions. This method requires only lepton energy distribution and ideally it does not depend on the velocity of the parent particle. We…

High Energy Physics - Phenomenology · Physics 2013-09-11 S. Kawabata , Y. Shimizu , Y. Sumino , H. Yokoya

The threshold scan at future lepton colliders is the most precise known method to determine the top quark mass (well below 100 MeV), a fundamental parameter of the Standard Model that co-determines the stability properties of the…

High Energy Physics - Phenomenology · Physics 2018-11-12 Jürgen Reuter , Bijan Chokoufé Nejad , Andre Hoang , Wolfgang Kilian , Maximilian Stahlhofen , Thomas Teubner , Christian Weiss

First observed in 1995, the top quark is one of a pair of third-generation quarks in the Standard Model of particle physics. It has charge +2/3e and a mass of 171.4 GeV, about 40 times heavier than its partner, the bottom quark. The CDF and…

High Energy Physics - Experiment · Physics 2019-08-15 A. P. Heinson