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The unpolarized, helicity and transversity distributions of quarks in the proton are calculated in the overlap representation of light-cone wavefunctions truncated to the lowest order Fock-space components with three valence quarks. The…

High Energy Physics - Phenomenology · Physics 2008-11-26 B. Pasquini , M. Pincetti , S. Boffi

This paper presents a measurement of the triple-differential cross section for the Drell--Yan process $Z/\gamma^*\rightarrow \ell^+\ell^-$ where $\ell$ is an electron or a muon. The measurement is performed for invariant masses of the…

High Energy Physics - Experiment · Physics 2018-02-12 ATLAS Collaboration

The Drell-Yan process is a copious source of lepton pairs at high energy and is measured with great precision at the Large Hadron Collider (LHC). Barring any new light particles, beyond the Standard Model effects can be studied in Drell-Yan…

High Energy Physics - Phenomenology · Physics 2019-03-06 S. Dawson , P. P. Giardino , A. Ismail

We compute for the first time the lepton-pair rapidity distribution in the photon-mediated Drell-Yan process to next-to-next-to-next-to-leading order (N$^3$LO) in QCD. The calculation is based on the qT-subtraction method, suitably extended…

High Energy Physics - Phenomenology · Physics 2022-02-04 Xuan Chen , Thomas Gehrmann , Nigel Glover , Alexander Huss , Tong-Zhi Yang , Hua Xing Zhu

We present a comprehensive comparison of the available experimental data for the Drell-Yan lepton angular coefficients $\lambda$ and $\nu$ to calculations at leading and next-to-leading order of perturbative QCD. To obtain the…

High Energy Physics - Phenomenology · Physics 2016-09-13 Martin Lambertsen , Werner Vogelsang

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. 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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 briefly discuss the collinear factorization formula for the associated production of one particle and a Drell-Yan pair in hadronic collisions. We outline possible applications of the results to three different research areas.

High Energy Physics - Phenomenology · Physics 2011-02-15 Federico Alberto Ceccopieri

The factorization theorems for transverse momentum distributions of dilepton/boson production, recently formulated by Collins and Echevarria-Idilbi-Scimemi in terms of well-defined transverse momentum dependent distributions (TMDs), allows…

High Energy Physics - Phenomenology · Physics 2015-06-22 Umberto D'Alesio , Miguel G. Echevarria , Stefano Melis , Ignazio Scimemi

We compute the rapidity distribution of the virtual photon produced in the Drell-Yan process through next-to-next-to-leading order in perturbative QCD. We introduce a powerful new method for calculating differential distributions in hard…

High Energy Physics - Phenomenology · Physics 2008-11-26 Charalampos Anastasiou , Lance Dixon , Kirill Melnikov , Frank Petriello

A correct modelling of the underlying event in proton-proton collisions is important for the proper simulation of kinematic distributions of high-energy collisions. The ATLAS collaboration extended previous studies at 7 TeV with a leading…

High Energy Physics - Experiment · Physics 2016-08-18 Yuri Kulchitsky

Transverse Momentum Dependent (TMD) parton distributions obtained from the Parton Branching (PB) method are combined with next-to-leading-order (NLO) calculations of Drell-Yan (DY) production. We apply the MCatNLO method for the hard…

We discuss the angular distribution of the lepton pair in the Drell-Yan process, hadron+hadron -> \gamma^* X -> l^+ l^- X. This process gives information on the spin-density matrix \rho^{(q,\bar{q})} of the annihilating quark-antiquark pair…

High Energy Physics - Phenomenology · Physics 2009-11-10 D. Boer , A. Brandenburg , O. Nachtmann , A. Utermann

We compute for the first time the complete corrections at N$^3$LO in the strong coupling constant to the inclusive neutral-current Drell-Yan process including contributions from both photon and $Z$-boson exchange. Our main result is the…

High Energy Physics - Phenomenology · Physics 2022-04-13 Claude Duhr , Bernhard Mistlberger

By measuring Drell-Yan massive lepton-pair's angular distributions, we can identify the polarization of the virtual photon of invariant mass $Q$ which decays immediately into the lepton-pair. In terms of a modified QCD factorization formula…

High Energy Physics - Phenomenology · Physics 2011-03-23 Jianwei Qiu , Ricardo Rodriguez , Xiaofei Zhang

We analyse polarised Drell-Yan process using the factorisation method and derive operator definitions for polarised parton distribution functions. We demonstrate that a factorisation analogous to that in the unpolarised Drell-Yan case holds…

High Energy Physics - Phenomenology · Physics 2015-06-25 Prakash Mathews , V. Ravindran

We discuss the nuclear parton distribution functions on the basis of our recently developed semi-microscopic model, which takes into account a number of nuclear effects including Fermi motion and nuclear binding, nuclear meson-exchange…

High Energy Physics - Phenomenology · Physics 2015-12-11 S. A. Kulagin , R. Petti

Calculations of Drell-Yan (DY) production at next-to-leading (NLO) order have been combined with Transverse Momentum Dependent (TMD) distributions obtained with the Parton Branching (PB). The predictions show a remarkable agreement with DY…

We study angular distributions in the Drell-Yan process using an extended transverse momentum dependent (TMD) factorization framework that includes kinematic power corrections. This approach allows the description of observables previously…

High Energy Physics - Phenomenology · Physics 2025-05-19 Alexey Vladimirov

The longitudinally polarized Drell-Yan process is one of most powerful tools to probe the structure of hadrons. By means of the recent formalism of the polarized proton-deuteron(pd) Drell-Yan, we calculate the ratio of the proton-deuteron…

High Energy Physics - Phenomenology · Physics 2010-01-15 Chun-Gui Duan , Li-Jie Shi , Peng-Nian Shen , Guang-Lie Li

The transverse momentum dependent parton distribution/fragmentation functions (TMDs) are essential in the factorization of a number of processes like Drell-Yan scattering, vector boson production, semi-inclusive deep inelastic scattering,…

High Energy Physics - Phenomenology · Physics 2018-06-05 Miguel G. Echevarria , Ignazio Scimemi , Alexey Vladimirov
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