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Since the discovery of the top quark in 1995 by the CDF and D0 collaborations at the Fermilab Tevatron proton antiproton collider, precise measurements of its mass are ongoing. Using data recorded by the D0 and CDF experiment, corresponding…

High Energy Physics - Experiment · Physics 2019-08-14 Reinhild Yvonne Peters

Assuming that a non-standard neutral Higgs with an enhanced Yukawa coupling to a bottom quark is observed at future hadron experiments, we propose a method for a better understanding of the Higgs sector. Our procedure is based on "counting"…

High Energy Physics - Phenomenology · Physics 2009-11-10 David Atwood , Shaouly Bar-Shalom , Gad Eilam , Amarjit Soni

A technique for separating top quark production from Standard Model background events is introduced. It is applicable to the channel in which one top quark decays semi-leptonically and its anti-quark decays hadronically into three jets, or…

High Energy Physics - Phenomenology · Physics 2010-11-01 Gary R. Goldstein , K. Sliwa , R. H. Dalitz

Ten years after its discovery at the Tevatron collider, we still know little about the top quark. Its large mass suggests it may play a key role in the mechanism of Electroweak Symmetry Breaking (EWSB), or open a window of sensitivity to…

High Energy Physics - Experiment · Physics 2010-04-22 A. Juste

We study the signal from the pair production of $t$-squarks at the Tevatron under the assumption that their two-body decay to charginos as well as their three-body decay to $W$ bosons is kinematically forbidden. In this case, the stop…

High Energy Physics - Phenomenology · Physics 2007-05-23 H. Baer , J. Sender , X. Tata

O(100 GeV) physics beyond the standard model (BSM) could be overlooked provided that it is hidden in the untouched Higgs sector or jets. The top quark forward-backward asymmetry measurements and di-jet bump, which is observed in the…

High Energy Physics - Phenomenology · Physics 2015-03-19 Xiao-ping Wang , Jia Xu , Shou-hua Zhu

The mass of the top quark is measured using top-antitop-quark pair events with high transverse momentum top quarks. The dataset, collected with the ATLAS detector in proton--proton collisions at $\sqrt{s}=13$ TeV delivered by the Large…

High Energy Physics - Experiment · Physics 2025-06-16 ATLAS Collaboration

The top quark is the heaviest known elementary particle. Observed for the first time in 1995 at the Tevatron by the CDF and D0 experiments, it has become object of several studies aimed at fully characterize its properties and decays.…

High Energy Physics - Experiment · Physics 2015-06-11 V. Chiochia

We measure the top quark mass in dilepton final states of top-antitop events in proton-antiproton collisions at sqrt(s) = 1.96 TeV, using data corresponding to an integrated luminosity of 9.7 fb^-1 at the Fermilab Tevatron Collider. The…

High Energy Physics - Experiment · Physics 2016-03-09 D0 Collaboration

A precision measurement of the top quark mass m_t is obtained using a sample of ttbar events from ppbar collisions at the Fermilab Tevatron with the CDF II detector. Selected events require an electron or muon, large missing transverse…

High Energy Physics - Experiment · Physics 2010-12-28 T. Aaltonen et al.

The top quark mass measurement with ATLAS in the lepton plus jets channel is summarized from the perspective of the early data. Using the invariant mass of the three jets arising from the hadronic side as the estimator of the top quark…

High Energy Physics - Experiment · Physics 2009-08-24 Antoine Marzin

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

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

An analysis is presented of events containing jets including at least one $b$-tagged jet, sizable missing transverse momentum, and at least two charged leptons including a pair of the same electric charge, with the scalar sum of the jet and…

High Energy Physics - Experiment · Physics 2016-11-22 Cecile Deterre

With the full Tevatron Run II and early LHC data samples, the opportunity for furthering our understanding of the properties of the top quark has never been more promising. Although the current knowledge of the top quark comes largely from…

High Energy Physics - Experiment · Physics 2015-06-03 Kevin Lannon , Fabrizio Margaroli , Chris Neu

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

The top quark is the most recently discovered of the standard model quarks, and because of its very large mass, studies of the top quark and its interactions are important both as tests of the standard model and as searches for new physical…

High Energy Physics - Experiment · Physics 2019-08-14 David J. Mietlicki

We consider the recent measurement of the top quark forward-backward asymmetry at the Fermilab Tevatron, which shows a discrepancy of slightly more than 2$\sigma$ compared to the SM prediction. We find that $t$-channel exchange of a color…

High Energy Physics - Phenomenology · Physics 2010-12-09 Jing Shu , Tim M. P. Tait , Kai Wang

We present the first experimental discrimination between the 2e/3 and 4e/3 top quark electric charge scenarios, using top quark pairs (ttbar) produced in ppbar collisions at sqrt{s}=1.96 TeV by the Fermilab Tevatron collider. We use 370…

High Energy Physics - Experiment · Physics 2008-11-26 D0 Collaboration , V. Abazov

The mass of the top quark is measured in a data set corresponding to 4.6 fb$^{-1}$ of proton-proton collisions with centre-of-mass energy $\sqrt{s}=7$ TeV collected by the ATLAS detector at the LHC. Events consistent with hadronic decays of…

High Energy Physics - Experiment · Physics 2015-04-29 ATLAS Collaboration