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Related papers: Inverse bremsstrahlung contributions to Drell-Yan …

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At high energies, Drell-Yan (DY) dilepton production viewed in the target rest frame should be interpreted as bremsstrahlung and can be expressed in terms of the same color dipole cross section as DIS. We compute DY cross sections on a…

High Energy Physics - Phenomenology · Physics 2009-10-31 B. Z. Kopeliovich , J. Raufeisen , A. V. Tarasov

We study the Drell-Yan process mediated by a new bosonic resonance at the LHC. The bosons of spin-0, 1, and 2 with the most general leading-order couplings to Standard Model fermions and gluons are considered, which provide a…

High Energy Physics - Phenomenology · Physics 2013-05-30 Cheng-Wei Chiang , Neil D. Christensen , Gui-Jun Ding , Tao Han

The T-odd leptons predicted by the littlest $Higgs$ model with T-parity can be pair produced via the subprocesses $gg\to \ell^{+}_{H}\ell^{-}_{H}$, $q\bar{q}\to \ell^{+}_{H}\ell^{-}_{H}$, $\gamma\gamma\to \ell^{+}_{H}\ell^{-}_{H}$ and $ VV…

High Energy Physics - Phenomenology · Physics 2009-11-19 Chong-Xing Yue , Yong-Zhi Wang , Wei Lui , Wei Ma

Significant differences between transverse and longitudinal polarized parton distributions are found at low energies within a light-front covariant quark model of the nucleon. These differences are due to relativistic spin effects…

High Energy Physics - Phenomenology · Physics 2009-10-31 F. Cano , P. Faccioli , M. Traini

The complete set of electroweak O(alpha) corrections to the Drell--Yan-like production of W bosons is calculated and compared to an approximation provided by the leading term of an expansion about the W-resonance pole. All relevant formulae…

High Energy Physics - Phenomenology · Physics 2009-09-25 Stefan Dittmaier , Michael Kramer

We apply the leading and sub-leading electroweak (EW) corrections to the Drell-Yan process of the neutralino pair production at proton-proton collision, in order to calculate the effects of the these corrections on the neutralino pair…

High Energy Physics - Phenomenology · Physics 2013-07-16 A. I. Ahmadov , M. Demirci

A study of the order $\alpha_s^2$ corrections to the Drell Yan (non-singlet) cross section for incoming states of arbitrary longitudinal helicities is presented. The study is performed in the case of the transverse momentum distributions,…

High Energy Physics - Phenomenology · Physics 2014-11-17 Sanghyeon Chang , Claudio Coriano , R. D. Field , L. E. Gordon

We study the renormalization of the Wilson loop with a path corresponding to the Drell-Yan lepton pair production in two-loop approximation of perturbation theory. We establish the renormalization group equation in next-to-leading order and…

High Energy Physics - Phenomenology · Physics 2009-10-31 A. V. Belitsky

We summarize the status of calculations of the electroweak radiative corrections to W and Z boson production via the Drell-Yan mechanism at hadron colliders. To fully exploit the precision physics potential of the high-luminosity…

High Energy Physics - Phenomenology · Physics 2009-11-07 U. Baur , D. Wackeroth

We report on the computation of the angle-between-leptons distribution in Drell-Yan processes. More precisely we study the recently introduced variable phi*, which provides us with a more accurate probe of the low Q_T domain of Z boson…

High Energy Physics - Phenomenology · Physics 2011-07-04 Simone Marzani , Andrea Banfi , Mrinal Dasgupta , Lee Tomlinson

We discuss the transverse momentum Q_T distribution of Drell-Yan pair, produced in collisions of transversely polarized protons. We calculate the transversely polarized Drell-Yan cross section up to order \alpha_s in the dimensional…

High Energy Physics - Phenomenology · Physics 2009-11-11 Hiroyuki Kawamura , Jiro Kodaira , Hirotaka Shimizu , Kazuhiro Tanaka

A parton-model description of high-energy hadronic interactions in the presence of Lorentz violation is presented. This approach is used to study lepton-hadron and hadron-hadron interactions at large momentum transfer. Cross sections for…

High Energy Physics - Phenomenology · Physics 2019-11-19 Nathan Sherrill

The production of lepton pairs at low invariant mass and finite transverse momentum resolves QCD dynamics at the boundary between the perturbative and non-perturbative domains. We investigate the impact of NNLO QCD corrections on these…

High Energy Physics - Phenomenology · Physics 2022-04-20 R. Gauld , A. Gehrmann-De Ridder , T. Gehrmann , E. W. N. Glover , A. Huss , I. Majer , A. Rodriguez Garcia

We discuss kinematical correlations between charged leptons from semileptonic decays of open charm/bottom, leptons produced in the Drell-Yan mechanism as well as some other mechanisms not included so far in the literature in proton-proton…

High Energy Physics - Phenomenology · Physics 2011-04-04 Rafal Maciula , Antoni Szczurek , Gabriela Slipek

The processes of lepton-nucleon scattering, including ones with both polarized beams, at high energy provide relevant information about interaction and particles structure, allowing to analyze nucleon spin structure. As energy and…

High Energy Physics - Phenomenology · Physics 2007-08-21 S. N. Sevbitov , T. V. Shishkina

We consider the transverse-momentum ($q_T$) distribution of Drell-Yan lepton pairs produced with invariant masses ($M$) from low values up to the $Z$-boson peak ($4\leq M \leq 116$~GeV). We present perturbative predictions obtained by…

High Energy Physics - Phenomenology · Physics 2026-01-27 Stefano Camarda , Giancarlo Ferrera , Lorenzo Rossi

Radiative corrections to the charged current Drell-Yan processes are revisited. Complete one-loop electroweak corrections are calculated within the automatic SANC system. Electroweak scheme dependence and the choice of the factorization…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Arbuzov , D. Bardin , S. Bondarenko , P. Christova , L. Kalinovskaya , G. Nanava , R. Sadykov

We review the development in the field of lepton pair production since proposing parton-antiparton annihilation as the mechanism of massive lepton pair production. The basic physical picture of the Drell-Yan model has survived the test of…

High Energy Physics - Phenomenology · Physics 2007-05-23 T-M. Yan

We study the underlying event in proton-antiproton collisions by examining the behavior of charged particles (transverse momentum pT > 0.5 GeV/c, pseudorapidity |\eta| < 1) produced in association with large transverse momentum jets (~2.2…

High Energy Physics - Experiment · Physics 2012-04-20 The CDF Collaboration , T. Aaltonen , J. Adelman , B. Alvarez Gonzalez , S. Amerio , D. Amidei , A. Anastassov , A. Annovi , J. Antos , G. Apollinari , A. Apresyan , T. Arisawa , A. Artikov , J. Asaadi , W. Ashmanskas , A. Attal , A. Aurisano , F. Azfar , W. Badgett , A. Barbaro-Galtieri , V. E. Barnes , B. A. Barnett , P. Barria , P. Bartos , G. Bauer , P. -H. Beauchemin , F. Bedeschi , D. Beecher , S. Behari , G. Bellettini , J. Bellinger , D. Benjamin , A. Beretvas , D. Berge , A. Bhatti , M. Binkley , D. Bisello , I. Bizjak , R. E. Blair , C. Blocker , B. Blumenfeld , A. Bocci , A. Bodek , V. Boisvert , D. Bortoletto , J. Boudreau , A. Boveia , B. Brau , A. Bridgeman , L. Brigliadori , C. Bromberg , E. Brubaker , J. Budagov , H. S. Budd , S. Budd , K. Burkett , G. Busetto , P. Bussey , A. Buzatu , K. L. Byrum , S. Cabrera , C. Calancha , S. Camarda , M. Campanelli , M. Campbell , F. Canelli , A. Canepa , B. Carls , D. Carlsmith , R. Carosi , S. Carrillon , S. Carron , B. Casal , M. Casarsa , A. Castrocc , P. Catastini , D. Cauz , V. Cavaliere , M. Cavalli-Sforza , A. Cerri , L. Cerrito , S. H. Chang , Y. C. Chen , M. Chertok , G. Chiarelli , G. Chlachidze , F. Chlebana , K. Cho , D. Chokheli , J. P. Chou , K. Chungo , W. H. Chung , Y. S. Chung , T. Chwalek , C. I. Ciobanu , M. A. Ciocci , A. Clark , D. Clark , G. Compostella , M. E. Convery , J. Conway , M. Corbo , M. Cordelli , C. A. Cox , D. J. Cox , F. Crescioli , C. Cuenca Almenar , J. Cuevas , R. Culbertson , J. C. Cully , D. Dagenhart , M. Datta , T. Davies , P. de Barbaro , S. De Cecco , A. Deisher , G. De Lorenzo , M. Dell'Orso , C. Deluca , L. Demortier , J. Deng , M. Deninno , M. d'Errico , A. Di Canto , G. P. di Giovanni , B. Di Ruzza , J. R. Dittmann , M. D'Onofrio , S. Donati , P. Dong , T. Dorigo , S. Dube , K. Ebina , A. Elagin , R. Erbacher , D. Errede , S. Errede , N. Ershaidat , R. Eusebi , H. C. Fang , S. Farrington , W. T. Fedorko , R. G. Feild , M. Feindt , J. P. Fernandez , C. Ferrazza , R. Field , G. Flanagans , R. Forrest , M. J. Frank , M. Franklin , J. C. Freeman , I. Furic , M. Gallinaro , J. Galyardt , F. Garberson , J. E. Garcia , A. F. Garfinkel , P. Garosi , H. Gerberich , D. Gerdes , A. Gessler , S. Giagu , V. Giakoumopoulou , P. Giannetti , K. Gibson , J. L. Gimmell , C. M. Ginsburg , N. Giokaris , M. Giordani , P. Giromini , M. Giunta , G. Giurgiu , V. Glagolev , D. Glenzinski , M. Gold , 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 , U. Grundler , J. Guimaraes da Costa , Z. Gunay-Unalan , C. Haber , S. R. Hahn , E. Halkiadakis , B. -Y. Han , J. Y. Han , F. Happacher , K. Hara , D. Hare , M. Hare , R. F. Harr , M. Hartz , K. Hatakeyama , C. Hays , M. Heck , J. Heinrich , M. Herndon , J. Heuser , S. Hewamanage , M. Hickman , D. Hidas , C. S. Hill , D. Hirschbuehl , A. Hocker , S. Hou , M. Houlden , S. -C. Hsu , R. E. Hughes , M. Hurwitz , U. Husemann , M. Hussein , J. Huston , J. Incandela , G. Introzzi , M. Iori , A. Ivanov , E. James , D. Jang , B. Jayatilaka , E. J. Jeon , M. K. Jha , S. Jindariani , W. Johnson , M. Jones , K. K. Joo , S. Y. Jun , J. E. Jung , T. R. Junk , T. Kamon , D. Kar , P. E. Karchin , Y. Kato , R. Kephart , 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 , L. Kirsch , S. Klimenko , K. Kondo , D. J. Kong , J. Konigsberg , A. Korytov , A. V. Kotwal , M. Kreps , J. Kroll , D. Krop , N. Krumnack , M. Kruse , V. Krutelyov , T. Kuhr , N. P. Kulkarni , M. Kurata , S. Kwang , A. T. Laasanen , S. Lami , S. Lammel , M. Lancaster , R. L. Lander , K. Lannon , A. Lath , G. Latino , I. Lazzizzera , T. LeCompte , E. Lee , H. S. Lee , J. S. Lee , S. W. Lee , S. Leone , J. D. Lewis , C. -J. Lin , J. Linacre , M. Lindgren , E. Lipeles , A. Lister , D. O. Litvintsev , C. Liu , T. Liu , N. S. Lockyer , A. Loginov , L. Lovas , D. Lucchesi , J. Lueck , P. Lujan , P. Lukens , G. Lungu , J. Lys , R. Lysak , D. MacQueen , R. Madrak , K. Maeshima , K. Makhoul , P. Maksimovic , S. Malde , S. Malik , G. Manca , A. Manousakis-Katsikakis , F. Margaroli , C. Marino , C. P. Marino , A. Martin , V. Martink , M. Martinez , R. Martinez-Ballarin , P. Mastrandrea , M. Mathis , M. E. Mattson , P. Mazzanti , K. S. McFarland , P. McIntyre , R. McNulty , A. Mehta , P. Mehtala , A. Menzione , C. Mesropian , T. Miao , D. Mietlicki , N. Miladinovic , R. Miller , C. Mills , M. Milnik , A. Mitra , G. Mitselmakher , H. Miyake , S. Moed , N. Moggi , M. N. Mondragon , C. S. Moon , R. Moore , M. J. Morello , J. Morlock , P. Movilla Fernandez , J. Mulmenstadt , A. Mukherjee , Th. Muller , P. Murat , M. Mussini , J. Nachtman , Y. Nagai , J. Naganoma , K. Nakamura , Nakano , A. Napier , J. Nett , C. Neu , M. S. Neubauer , S. Neubauer , J. Nielseng , L. Nodulman , M. Norman , O. Norniella , E. Nurse , L. Oakes , S. H. Oh , Y. D. Oh , I. Oksuzian , T. Okusawa , R. Orava , K. Osterberg , S. Pagan Griso , C. Pagliarone , E. Palencia , V. Papadimitriou , A. Papaikonomou , A. A. Paramanov , B. Parks , S. Pashapour , J. Patrick , G. Pauletta , M. Paulini , C. Paus , T. Peiffer , D. E. Pellett , A. Penzo , T. J. Phillips , G. Piacentino , E. Pianori , L. Pinera , K. Pitts , C. Plager , L. Pondrom , K. Potamianos , O. Poukhov , F. Prokoshin , A. Pronko , F. Ptohos , E. Pueschel , G. Punzi , J. Pursley , J. Rademacker , A. Rahaman , V. Ramakrishnan , N. Ranjan , I. Redondo , P. Renton , M. Renz , M. Rescigno , S. Richter , F. Rimondi , L. Ristori , A. Robson , T. Rodrigo , T. Rodriguez , E. Rogers , S. Rolli , R. Roser , M. Rossi , R. Rossin , P. Roy , A. Ruiz , J. Russ , V. Rusu , B. Rutherford , H. Saarikko , A. Safonov , W. K. Sakumoto , L. Santi , L. Sartori , K. Sato , A. Savoy-Navarro , P. Schlabach , A. Schmidt , E. E. Schmidt , M. A. Schmidt , M. P. Schmidt , M. Schmitt , T. Schwarz , L. Scodellaro , A. Scribano , F. Scuri , A. Sedov , S. Seidel , Y. Seiya , A. Semenov , L. Sexton-Kennedy , F. Sforza , A. Sfyrla , S. Z. Shalhout , T. Shears , P. F. Shepard , M. Shimojima , S. Shiraishi , M. Shochet , Y. Shon , I. Shreyber , A. Simonenko , P. Sinervo , A. Sisakyan , A. J. Slaughter , J. Slaunwhite , K. Sliwa , J. R. Smith , F. D. Snider , R. Snihur , 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 , J. S. Suh , A. Sukhanov , I. Suslov , A. Taffard , R. Takashima , Y. Takeuchi , R. Tanaka , J. Tang , M. Tecchio , P. K. Teng , J. Thom , J. Thome , G. A. Thompson , E. Thomson , P. Tipton , P. Ttito-Guzmán , S. Tkaczyk , D. Toback , S. Tokar , K. Tollefson , T. Tomura , D. Tonelli , S. Torre , D. Torretta , P. Totaro , S. Tourneur , M. Trovato , S. -Y. Tsai , Y. Tu , N. Turiniff , F. Ukegawa , S. Uozumi , N. van Remortel , A. Varganov , E. Vataga , F. Vázquez , G. Velev , C. Vellidis , M. Vidal , I. Vila , R. Vilar , M. Vogel , I. Volobouev , G. Volpi , P. Wagner , R. G. Wagner , R. L. Wagner , W. Wagner , J. Wagner-Kuhr , T. Wakisaka , R. Wallny , S. M. Wang , A. Warburton , D. Waters , M. Weinberger , J. Weinelt , W. C. Wester , B. Whitehouse , D. Whiteson , A. B. Wicklund , E. Wicklund , S. Wilbur , G. Williams , H. H. Williams , M. G. Wilson , P. Wilson , B. L. Winer , P. Wittich , S. Wolbers , C. Wolfe , H. Wolfe , T. Wright , X. Wu , F. Würthwein , A. Yagil , K. Yamamoto , J. Yamaoka , U. K. Yang , Y. C. Yang , W. M. Yao , G. P. Yeh , K. Yio , J. Yoh , K. Yorita , T. Yoshidal , G. B. Yu , I. Yu , S. S. Yu , J. C. Yun , A. Zanetti , Y. Zeng , X. Zhang , Y. Zheng , S. Zucchelli

We calculate the complete electroweak O(alpha) corrections to pp, pbar p -> l+l- X (l=e, mu) in the Standard Model of electroweak interactions. They comprise weak and photonic virtual one-loop corrections as well as real photon radiation to…

High Energy Physics - Phenomenology · Physics 2010-04-06 U. Baur , O. Brein , W. Hollik , C. Schappacher , D. Wackeroth