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After a brief review of the production dynamics of prompt single photons in hadron collisions, I summarize a new QCD calculation of the transverse momentum distribution of continuum prompt photon pairs produced by QCD subprocesses,…

High Energy Physics - Phenomenology · Physics 2014-11-18 Edmond L. Berger

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

In the Minimal Supersymmetric Standard Model, one of the scalar top quarks can be relatively light and its couplings to Higgs bosons strongly enhanced. I will discuss two consequences of this feature: 1) the effects of scalar top loops on…

High Energy Physics - Phenomenology · Physics 2007-05-23 Abdelhak Djouadi

We compute, in the framework of renormalon calculus, the ${\cal O}(\Lambda_{\rm QCD})$ corrections to the production of $t\bar{t}$ pairs in hadron collisions under the assumption that $q \bar q \to t \bar t$ is the dominant partonic…

High Energy Physics - Phenomenology · Physics 2024-11-25 Sergei Makarov , Kirill Melnikov , Paolo Nason , Melih A. Ozcelik

I present a calculation of next-to-next-to-next-to-leading-order (NNNLO) soft-gluon corrections for differential distributions in top-antitop pair production in hadronic collisions. Approximate NNNLO (aNNNLO) results are obtained from…

High Energy Physics - Phenomenology · Physics 2015-03-05 Nikolaos Kidonakis

We present updated predictions for the total cross section of top-quark pair production at Tevatron and LHC. For the LHC we also provide results at sqrt(s) = 10 TeV, in view of the anticipated run in 2008 and quote numbers for the…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Moch , P. Uwer

Presented are complete next-to-leading order electroweak (NLO EW) corrections to top-squark pair production at the Large Hadron Collider (LHC) within the Minimal Supersymmetric Standard Model (MSSM). At this order, also effects from the…

High Energy Physics - Phenomenology · Physics 2009-02-18 Wolfgang Hollik , Monika Kollar , Maike K. Trenkel

We search for direct pair production of supersymmetric top quarks and supersymmetric bottom quarks in proton-antiproton collisions at sqrt(s)=1.96 TeV, using 295 pb^-1 of data recorded by the Collider Detector at Fermilab (CDF II)…

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

We present total rates and kinematic distributions for the associated production of a single bottom quark and a Higgs boson at the Tevatron and the LHC. We include next-to-leading order QCD corrections and compare the results obtained in…

High Energy Physics - Phenomenology · Physics 2009-11-10 S. Dawson , C. B. Jackson , L. Reina , D. Wackeroth

I present a calculation of soft-gluon corrections to single top quark production in pp collisions at the LHC via the Standard Model partonic processes in the t and s channels and associated top quark and W boson production. Higher-order…

High Energy Physics - Phenomenology · Physics 2008-11-26 Nikolaos Kidonakis

We propose techniques to observe the correlation of the spins of top quarks and antiquarks at the Tevatron and the LHC. Observation of the spin correlation would confirm that the top quark decays before its spin flips, and would place a…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. Stelzer , S. Willenbrock

I present the resummation of collinear and soft gluon corrections to single top quark production in the t channel at next-to-next-to-leading logarithm (NNLL) accuracy using two-loop soft anomalous dimensions. The expansion of the resummed…

High Energy Physics - Phenomenology · Physics 2011-05-25 Nikolaos Kidonakis

We consider transverse-momentum resummation for top-quark pair production in hadron collisions. At small transverse momenta of the top-quark pair, the logarithmically-enhanced QCD contributions are resummed to all orders up to…

High Energy Physics - Phenomenology · Physics 2018-12-05 Stefano Catani , Massimiliano Grazzini , Hayk Sargsyan

We compute the inclusive and differential cross sections for the associated production of a top quark along with a charged Higgs boson at hadron colliders to next-to-leading order (NLO) in perturbative quantum chromodynamics (QCD) and in…

High Energy Physics - Phenomenology · Physics 2009-11-10 Edmond L Berger , Tao Han , Jing Jiang , Tilman Plehn

In the context of the Minimal Supersymmetric extension of the Standard Model, I discuss the effects of relatively light top and bottom scalar quarks on the main production mechanism of the lightest SUSY neutral Higgs boson $h$ at the LHC,…

High Energy Physics - Phenomenology · Physics 2011-01-27 Abdelhak DJOUADI

We present new theoretical predictions for the t bar t production cross section at NNLO at the Tevatron and the LHC. We discuss the scale uncertainty and the errors due to the parton distribution functions (PDFs). For the LHC, we present a…

High Energy Physics - Phenomenology · Physics 2009-07-16 U. Langenfeld , S. Moch , P. Uwer

One of the main goals for hadron colliders is the study of the properties of the third generation quarks. We study the signatures for new TeV resonances that couple to top or bottom quarks both at the Tevatron Run II and at the LHC. We find…

High Energy Physics - Phenomenology · Physics 2009-11-10 T. Han , G. Valencia , Yili Wang

The production of a top-antitop quark pair in association with a $W$ boson ($t\bar tW$) is one of the heaviest signatures currently probed at the Large Hadron Collider (LHC). Since the first observation reported in 2015 the corresponding…

High Energy Physics - Phenomenology · Physics 2023-12-08 Luca Buonocore , Simone Devoto , Massimiliano Grazzini , Stefan Kallweit , Javier Mazzitelli , Luca Rottoli , Chiara Savoini

We present predictions for the total ttbar production cross section sigma_ttbar at the Tevatron and LHC, which include the resummation of soft logarithms and Coulomb singularities through next-to-next-to-leading logarithmic order, and ttbar…

High Energy Physics - Phenomenology · Physics 2011-12-21 M. Beneke , P. Falgari , S. Klein , C. Schwinn

We revisit the possibility that the top quark forward-backward asymmetry arises from the on-shell production and decay of scalar top partners to top-antitop pairs with missing transverse energy. Although the asymmetry is produced by…

High Energy Physics - Phenomenology · Physics 2013-11-22 Abhishek Kumar , John N. Ng , Andrew Spray , Peter T. Winslow
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