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The top quark was discovered at the Tevatron in 1995. For the last decade the study of its properties has been a major theme in the worldwide experimental high energy physics program. The advent of the LHC opens up a new era in top quark…

High Energy Physics - Experiment · Physics 2008-10-20 Jesus Manuel Vizan

\def\nle{{\stackrel{<}{\sim}}} We examine a possibility for existence of a light supersymmetric partner of the top quark (stop) with mass 15 $\sim$ 20 GeV in the framework of the minimal supergravity GUT model. Such light stop could explain…

High Energy Physics - Phenomenology · Physics 2009-10-22 Tadashi Kon , Toshihiko Nonaka

Top quarks are produced at the Tevatron proton-antiproton collider at Fermilab and at the Large Hadron (proton-proton) Collider at CERN in two ways: as quark-antiquark pairs, and singly. For each mode, the cross sections and future…

High Energy Physics - Experiment · Physics 2007-05-23 A. P. Heinson

Associated single top production with a Z boson or a photon at large hadron colliders provides a precise determination of top flavour-changing neutral couplings. The best way to measure these couplings with the up quark at Tevatron is to…

High Energy Physics - Phenomenology · Physics 2009-10-31 F. del Aguila , J. A. Aguilar-Saavedra , Ll. Ametller

A search for pair production of the lightest supersymmetric partner of the top quark is performed in the lepton+jets channel using 0.9 fb-1 of data collected by the D0 experiment. Kinematic differences between scalar top quark pair…

High Energy Physics - Experiment · Physics 2009-03-24 D0 Collaboration , V. Abazov

The results of a search for pair production of light top squarks are presented, using 4.7 fb^-1 of sqrt(s) = 7 TeV proton-proton collisions collected with the ATLAS detector at the Large Hadron Collider. This search targets top squarks with…

High Energy Physics - Experiment · Physics 2013-06-24 ATLAS Collaboration

We determine the constraints on the anomalous top-quark coupling associated with the flavor-changing neutral current vertex $\bar t c \gamma $ from the limits on the $b$-quark rare decay $b\rightarrow s \gamma$ and non-standard top-quark…

High Energy Physics - Phenomenology · Physics 2016-08-24 T. Han , K. Whisnant , B. -L. Young , X. Zhang

We study in detail the model by Isidori and Kamenik that is claimed to explain the top quark forward-backward asymmetry at Tevatron, provide GeV-scale dark matter (DM), and possibly improve the agreement between data and theory in Tevatron…

High Energy Physics - Phenomenology · Physics 2011-08-18 Andi Hektor , Gert Hütsi , Mario Kadastik , Kristjan Kannike , Martti Raidal , David M. Straub

We present a search for the pair production of scalar top quarks ($\tilde{t}_{1}$), the lightest supersymmetric partners of the top quarks, in $p\bar{p}$ collisions at a center-of-mass energy of 1.96 TeV, using data corresponding to an…

High Energy Physics - Experiment · Physics 2015-06-04 D0 Collaboration , V. M. Abazov , B. Abbott , B. S. Acharya , M. Adams , T. Adams , G. D. Alexeev , G. Alkhazov , A. Alton , G. Alverson , M. Aoki , A. Askew , B. Asman , S. Atkins , O. Atramentov , K. Augsten , C. Avila , J. BackusMayes , F. Badaud , L. Bagby , B. Baldin , D. V. Bandurin , S. Banerjee , E. Barberis , P. Baringer , J. Barreto , J. F. Bartlett , U. Bassler , V. Bazterra , A. Bean , M. Begalli , C. Belanger-Champagne , L. Bellantoni , S. B. Beri , G. Bernardi , R. Bernhard , I. Bertram , M. Besancon , R. Beuselinck , V. A. Bezzubov , P. C. Bhat , S. Bhatia , V. Bhatnagar , G. Blazey , S. Blessing , K. Bloom , A. Boehnlein , D. Boline , E. E. Boos , G. Borissov , T. Bose , A. Brandt , O. Brandt , R. Brock , G. Brooijmans , A. Bross , D. Brown , J. Brown , X. B. Bu , M. Buehler , V. Buescher , V. Bunichev , S. Burdin , T. H. Burnett , C. P. Buszello , B. Calpas , E. Camacho-Perez , M. A. Carrasco-Lizarraga , B. C. K. Casey , H. Castilla-Valdez , S. Chakrabarti , D. Chakraborty , K. M. Chan , A. Chandra , E. Chapon , G. Chen , S. Chevalier-Thery , D. K. Cho , S. W. Cho , S. Choi , B. Choudhary , S. Cihangir , D. Claes , J. Clutter , M. Cooke , W. E. Cooper , M. Corcoran , F. Couderc , M. -C. Cousinou , A. Croc , D. Cutts , A. Das , G. Davies , S. J. de Jong , E. De La Cruz-Burelo , F. Deliot , R. Demina , D. Denisov , S. P. Denisov , S. Desai , C. Deterre , K. DeVaughan , H. T. Diehl , M. Diesburg , P. F. Ding , A. Dominguez , T. Dorland , A. Dubey , L. V. Dudko , D. Duggan , A. Duperrin , S. Dutt , A. Dyshkant , M. Eads , D. Edmunds , J. Ellison , V. D. Elvira , Y. Enari , H. Evans , A. Evdokimov , V. N. Evdokimov , G. Facini , T. Ferbel , F. Fiedler , F. Filthaut , W. Fisher , H. E. Fisk , M. Fortner , H. Fox , S. Fuess , A. Garcia-Bellido , G. A. Garcia-Guerra , V. Gavrilov , P. Gay , W. Geng , D. Gerbaudo , C. E. Gerber , Y. Gershtein , G. Ginther , G. Golovanov , A. Goussiou , P. D. Grannis , S. Greder , H. Greenlee , Z. D. Greenwood , E. M. Gregores , G. Grenier , Ph. Gris , J. -F. Grivaz , A. Grohsjean , S. Grunendahl , M. W. Grunewald , T. Guillemin , G. Gutierrez , P. Gutierrez , A. Haas , S. Hagopian , J. Haley , L. Han , K. Harder , A. Harel , J. M. Hauptman , J. Hays , T. Head , T. Hebbeker , D. Hedin , H. Hegab , A. P. Heinson , U. Heintz , C. Hensel , I. Heredia-De La Cruz , K. Herner , G. Hesketh , M. D. Hildreth , R. Hirosky , T. Hoang , J. D. Hobbs , B. Hoeneisen , M. Hohlfeld , Z. Hubacek , V. Hynek , I. Iashvili , Y. Ilchenko , R. Illingworth , A. S. Ito , S. Jabeen , M. Jaffre , D. Jamin , A. Jayasinghe , R. Jesik , K. Johns , M. Johnson , A. Jonckheere , P. Jonsson , J. Joshi , A. W. Jung , A. Juste , K. Kaadze , E. Kajfasz , D. Karmanov , P. A. Kasper , I. Katsanos , R. Kehoe , S. Kermiche , N. Khalatyan , A. Khanov , A. Kharchilava , Y. N. Kharzheev , J. M. Kohli , A. V. Kozelov , J. Kraus , S. Kulikov , A. Kumar , A. Kupco , T. Kurca , V. A. Kuzmin , S. Lammers , G. Landsberg , P. Lebrun , H. S. Lee , S. W. Lee , W. M. Lee , J. Lellouch , H. Li , L. Li , Q. Z. Li , S. M. Lietti , J. K. Lim , D. Lincoln , J. Linnemann , V. V. Lipaev , R. Lipton , Y. Liu , A. Lobodenko , M. Lokajicek , R. Lopes de Sa , H. J. Lubatti , R. Luna-Garcia , A. L. Lyon , A. K. A. Maciel , D. Mackin , R. Madar , R. Magana-Villalba , S. Malik , V. L. Malyshev , Y. Maravin , J. Martinez-Ortega , R. McCarthy , C. L. McGivern , M. M. Meijer , A. Melnitchouk , D. Menezes , P. G. Mercadante , M. Merkin , A. Meyer , J. Meyer , F. Miconi , N. K. Mondal , G. S. Muanza , M. Mulhearn , E. Nagy , M. Naimuddin , M. Narain , R. Nayyar , H. A. Neal , J. P. Negret , P. Neustroev , S. F. Novaes , T. Nunnemann , G. Obrant , J. Orduna , N. Osman , J. Osta , G. J. Otero y Garzon , M. Padilla , A. Pal , N. Parashar , V. Parihar , S. K. Park , R. Partridge , N. Parua , A. Patwa , B. Penning , M. Perfilov , Y. Peters , K. Petridis , G. Petrillo , P. Petroff , R. Piegaia , M. -A. Pleier , P. L. M. Podesta-Lerma , V. M. Podstavkov , P. Polozov , A. V. Popov , M. Prewitt , D. Price , N. Prokopenko , J. Qian , A. Quadt , B. Quinn , M. S. Rangel , K. Ranjan , P. N. Ratoff , I. Razumov , P. Renkel , M. Rijssenbeek , I. Ripp-Baudot , F. Rizatdinova , M. Rominsky , A. Ross , C. Royon , P. Rubinov , R. Ruchti , G. Safronov , G. Sajot , P. Salcido , A. Sanchez-Hernandez , M. P. Sanders , B. Sanghi , A. S. Santos , G. Savage , L. Sawyer , T. Scanlon , R. D. Schamberger , Y. Scheglov , H. Schellman , T. Schliephake , S. Schlobohm , C. Schwanenberger , R. Schwienhorst , J. Sekaric , H. Severini , E. Shabalina , V. Shary , A. A. Shchukin , R. K. Shivpuri , V. Simak , V. Sirotenko , P. Skubic , P. Slattery , D. Smirnov , K. J. Smith , G. R. Snow , J. Snow , S. Snyder , S. Soldner-Rembold , L. Sonnenschein , K. Soustruznik , J. Stark , V. Stolin , D. A. Stoyanova , M. Strauss , D. Strom , L. Stutte , L. Suter , P. Svoisky , M. Takahashi , A. Tanasijczuk , M. Titov , V. V. Tokmenin , Y. -T. Tsai , K. Tschann-Grimm , D. Tsybychev , B. Tuchming , C. Tully , L. Uvarov , S. Uvarov , S. Uzunyan , R. Van Kooten , W. M. van Leeuwen , N. Varelas , E. W. Varnes , I. A. Vasilyev , P. Verdier , L. S. Vertogradov , M. Verzocchi , M. Vesterinen , D. Vilanova , P. Vokac , H. D. Wahl , M. H. L. S. Wang , J. Warchol , G. Watts , M. Wayne , M. Weber , J. Weichert , L. Welty-Rieger , A. White , D. Wicke , M. R. J. Williams , G. W. Wilson , M. Wobisch , D. R. Wood , T. R. Wyatt , Y. Xie , R. Yamada , W. -C. Yang , T. Yasuda , Y. A. Yatsunenko , W. Ye , Z. Ye , H. Yin , K. Yip , S. W. Youn , T. Zhao , B. Zhou , J. Zhu , M. Zielinski , D. Zieminska , L. Zivkovic

We present an analysis of dilepton events originating from top-antitop production in proton-antiproton collisions at sqrt{s}=1.8 TeV at the Fermilab Tevatron Collider. The sample corresponds to an integrated luminosity of 109+-7 pb^{-1}. We…

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

We report the latest results on the top-quark mass and on the top-antitop mass difference from the CDF and D0 collaborations using data collected at the Fermilab Tevatron $p\bar{p}$ collider at $\sqrt{s}=1.96$ TeV. We discuss general issues…

High Energy Physics - Experiment · Physics 2011-07-25 Zhenyu Ye , for CDF , D0 collaborations

The top quark is one of the least well-studied components of the standard model. In these lectures I discuss the expected properties of the top quark, which will be tested at the Fermilab Tevatron and the CERN Large Hadron Collider. I begin…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Willenbrock

I discuss the production of leptoquarks in $p\bar{p}$ collisions at the Fermilab Tevatron. Evaluated on the basis of a recent next-to-leading order calculation, the combined D0 and CDF leptoquark searches lead to a parameter-free lower mass…

High Energy Physics - Phenomenology · Physics 2008-02-03 Michael Krämer

We report precision measurements of the top quark mass using events collected by the D{\O}and CDF II detectors from $p\bar{p}$ collisions at $\sqrt s = 1.96$ TeV at the Fermilab Tevatron. Measurements are presented in multiple decay…

High Energy Physics - Experiment · Physics 2007-05-23 Daniel Whiteson

Charged Higgs scalars light enough to contribute to top quark decays are possible in various non--minimal Higgs models. We show that such a decay would be consistent with the current Tevatron data, and will remain hidden until a larger…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. G. Akeroyd

A number of top-spin observables are computed within the Standard Model (SM), at next-to-leading order in the strong and weak gauge couplings for hadronic top-quark anti-quark (ttbar) production and decay at the LHC for center-of-mass…

High Energy Physics - Phenomenology · Physics 2015-06-15 Werner Bernreuther , Zong-Guo Si

Two of the most important parameters in supersymmetry are the masses of the stop and sbottom, the supersymmetric partners of the third generation quarks. A stop mass lighter than 1 TeV is favored theoretically, however, conventional…

High Energy Physics - Experiment · Physics 2017-09-05 Keisuke Yoshihara

The CDF and D0 collaborations at Fermilab's Tevatron p-pbar collider have in place an extensive program to measure fundamental properties of the top quark. Recent results from Run I (sqrt-s = 1.8 TeV) and Run II (sqrt-s = 1.96 TeV) on the…

High Energy Physics - Experiment · Physics 2010-04-22 Andy Hocker

We analyze the two decays $\thb$, $\tstn$ within the Minimal Supersymmetric Standard Model with radiative breaking of the electroweak sector. We discuss their detectability at present and in the eventuality that supersymmetry is not…

High Energy Physics - Phenomenology · Physics 2008-02-03 Francesc M. Borzumati , N. Polonsky

The ATLAS and CMS experiments at the CERN LHC have collected about 20 $fb^{-1}$ of data each at the end of their 8 TeV run, and ruled out a huge swath of parameter space in the context of Minimally Supersymmetric Standard Model(MSSM).…

High Energy Physics - Phenomenology · Physics 2013-10-29 Amit Chakraborty , Dilip Kumar Ghosh , Diptimoy Ghosh , Dipan Sengupta