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Related papers: MILOU : a Monte-Carlo for Deeply Virtual Compton S…

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We present the calculation for single-inclusive jet production in (longitudinally) polarized deep-inelastic lepton-nucleon scattering at next-to-next-to leading order (NNLO) accuracy, based on the Projection-to-Born method. As a necessary…

High Energy Physics - Phenomenology · Physics 2021-01-13 Ignacio Borsa , Daniel de Florian , Iván Pedron

In 2011 Radyushkin outlined the practical implementation of the One-Component Double Distribution formalism in realistic Generalized Parton Distribution models. We compare the One-Component Double Distribution framework to the standard one…

High Energy Physics - Phenomenology · Physics 2013-08-09 C. Mezrag , H. Moutarde , F. Sabatié

Spin and transverse momentum dependent parton distributions - Generalized Parton Distributions (GPDs) - are at the interface between the QCD structure of the hadrons and observable quantities. The GPDs are linear superpositions within…

High Energy Physics - Phenomenology · Physics 2015-10-27 Gary R. Goldstein , Simonetta Liuti

Virtual Compton scattering off nucleons and pions at low energies is discussed. Predictions for the generalized polarizabilities of the nucleon are presented within the framework of heavy-baryon chiral perturbation theory and the linear…

High Energy Physics - Phenomenology · Physics 2011-04-15 S. Scherer

Virtual Compton Scattering (VCS) on the proton has been studied at Jefferson Lab using the exclusive photon electroproduction reaction (e p --> e p gamma). This paper gives a detailed account of the analysis which has led to the…

Nuclear Experiment · Physics 2013-05-30 H. Fonvieille , G. Laveissiere , N. Degrande , S. Jaminion , C. Jutier , L. Todor , R. Di Salvo , L. Van Hoorebeke , L. C. Alexa , B. D. Anderson , K. A. Aniol , K. Arundell , G. Audit , L. Auerbach , F. T. Baker , M. Baylac , J. Berthot , P. Y. Bertin , W. Bertozzi , L. Bimbot , W. U. Boeglin , E. J. Brash , V. Breton , H. Breuer , E. Burtin , J. R. Calarco , L. S. Cardman , C. Cavata , C. -C. Chang , J. -P. Chen , E. Chudakov , E. Cisbani , D. S. Dale , C. W. deJager , R. De Leo , A. Deur , N. d'Hose , G. E. Dodge , J. J. Domingo , L. Elouadrhiri , M. B. Epstein , L. A. Ewell , J. M. Finn , K. G. Fissum , G. Fournier , B. Frois , S. Frullani , C. Furget , H. Gao , J. Gao , F. Garibaldi , A. Gasparian , S. Gilad , R. Gilman , A. Glamazdin , C. Glashausser , J. Gomez , V. Gorbenko , P. Grenier , P. A. M. Guichon , J. O. Hansen , R. Holmes , M. Holtrop , C. Howell , G. M. Huber , C. E. Hyde , S. Incerti , M. Iodice , J. Jardillier , M. K. Jones , W. Kahl , S. Kato , A. T. Katramatou , J. J. Kelly , S. Kerhoas , A. Ketikyan , M. Khayat , K. Kino , S. Kox , L. H. Kramer , K. S. Kumar , G. Kumbartzki , M. Kuss , A. Leone , J. J. LeRose , M. Liang , R. A. Lindgren , N. Liyanage , G. J. Lolos , R. W. Lourie , R. Madey , K. Maeda , S. Malov , D. M. Manley , C. Marchand , D. Marchand , D. J. Margaziotis , P. Markowitz , J. Marroncle , J. Martino , K. McCormick , J. McIntyre , S. Mehrabyan , F. Merchez , Z. E. Meziani , R. Michaels , G. W. Miller , J. Y. Mougey , S. K. Nanda , D. Neyret , E. A. J. M. Offermann , Z. Papandreou , B. Pasquini , C. F. Perdrisat , R. Perrino , G. G. Petratos , S. Platchkov , R. Pomatsalyuk , D. L. Prout , V. A. Punjabi , T. Pussieux , G. Quemener , R. D. Ransome , O. Ravel , J. S. Real , F. Renard , Y. Roblin , D. Rowntree , G. Rutledge , P. M. Rutt , A. Saha , T. Saito , A. J. Sarty , A. Serdarevic , T. Smith , G. Smirnov , K. Soldi , P. Sorokin , P. A. Souder , R. Suleiman , J. A. Templon , T. Terasawa , R. Tieulent , E. Tomasi-Gustaffson , H. Tsubota , H. Ueno , P. E. Ulmer , G. M. Urciuoli , M. Vanderhaeghen , R. L. J. Van der Meer , R. Van De Vyver , P. Vernin , B. Vlahovic , H. Voskanyan , E. Voutier , J. W. Watson , L. B. Weinstein , K. Wijesooriya , R. Wilson , B. B. Wojtsekhowski , D. G. Zainea , W. -M. Zhang , J. Zhao , Z. -L. Zhou

The key reactions to study the Generalised Parton Distributions are Deeply Virtual Compton Scattering (DVCS) and Deeply Virtual Meson Production (DVMP). At COMPASS, these processes are investigated using a high intensity muon beam with a…

High Energy Physics - Experiment · Physics 2017-02-22 P. Joerg

We report on the first measurement of exclusive single-photon muoproduction on the proton by COMPASS using 160 GeV/$c$ polarized $\mu^+$ and $\mu^-$ beams of the CERN SPS impinging on a liquid hydrogen target. We determine the dependence of…

High Energy Physics - Experiment · Physics 2019-12-12 R. Akhunzyanov , M. G. Alexeev , G. D. Alexeev , A. Amoroso , V. Andrieux , N. V. Anfimov , V. Anosov , A. Antoshkin , K. Augsten , W. Augustyniak , A. Austregesilo , C. D. R. Azevedo , B. Badelek , F. Balestra , M. Ball , J. Barth , R. Beck , Y. Bedfer , J. Bernhard , K. Bicker , E. R. Bielert , R. Birsa , M. Bodlak , P. Bordalo , F. Bradamante , A. Bressan , M. Buechele , E. Burtin , V. E. Burtsev , W. -C. Chang , C. Chatterjee , M. Chiosso , I. Choi , A. G. Chumakov , S. -U. Chung , A. Cicuttin , M. L. Crespo , S. Dalla Torre , S. S. Dasgupta , S. Dasgupta , O. Yu. Denisov , L. Dhara , S. V. Donskov , N. Doshita , Ch. Dreisbach , W. Duennweber , R. R. Dusaev , M. Dziewiecki , A. Efremov , P. D. Eversheim , M. Faessler , A. Ferrero , M. Finger , M. Finger , H. Fischer , C. Franco , N. du Fresne von Hohenesche , J. M. Friedrich , V. Frolov , E. Fuchey , F. Gautheron , O. P. Gavrichtchouk , S. Gerassimov , J. Giarra , I. Gnesi , M. Gorzellik , A. Grasso , A. Gridin , M. Grosse Perdekamp , B. Grube , T. Grussenmeyer , A. Guskov , D. Hahne , G. Hamar , D. von Harrach , R. Heitz , F. Herrmann , N. Horikawa , N. d'Hose , C. -Y. Hsieh , S. Huber , S. Ishimoto , A. Ivanov , Yu. Ivanshin , T. Iwata , V. Jary , R. Joosten , P. Joerg , K. Juraskova , E. Kabuss , A. Kerbizi , B. Ketzer , G. V. Khaustov , Yu. A. Khokhlov , Yu. Kisselev , F. Klein , J. H. Koivuniemi , V. N. Kolosov , K. Kondo , I. Konorov , V. F. Konstantinov , A. M. Kotzinian , O. M. Kouznetsov , Z. Kral , M. Kraemer , F. Krinner , Z. V. Kroumchtein , Y. Kulinich , F. Kunne , K. Kurek , R. P. Kurjata , I. I. Kuznetsov , A. Kveton , A. A. Lednev , E. A. Levchenko , M. Levillain , S. Levorato , Y. -S. Lian , J. Lichtenstadt , R. Longo , V. E. Lyubovitskij , A. Maggiora , A. Magnon , N. Makins , N. Makke , G. K. Mallot , S. A. Mamon , C. Marchand , B. Marianski , A. Martin , J. Marzec , J. Matousek , H. Matsuda , T. Matsuda , G. V. Meshcheryakov , M. Meyer , W. Meyer , Yu. V. Mikhailov , M. Mikhasenko , E. Mitrofanov , N. Mitrofanov , Y. Miyachi , A. Moretti , A. Nagaytsev , F. Nerling , D. Neyret , J. Novy , W. -D. Nowak , G. Nukazuka , A. S. Nunes , A. G. Olshevsky , I. Orlov , M. Ostrick , D. Panzieri , B. Parsamyan , S. Paul , J. -C. Peng , F. Pereira , G. Pesaro , M. Pesek , M. Peskova , D. V. Peshekhonov , N. Pierre , S. Platchkov , J. Pochodzalla , V. A. Polyakov , J. Pretz , M. Quaresma , C. Quintans , S. Ramos , C. Regali , G. Reicherz , C. Riedl , N. S. Rogacheva , D. I. Ryabchikov , A. Rybnikov , A. Rychter , R. Salac , V. D. Samoylenko , A. Sandacz , C. Santos , S. Sarkar , I. A. Savin , T. Sawada , G. Sbrizzai , P. Schiavon , H. Schmieden , K. Schoennig , E. Seder , A. Selyunin , L. Silva , L. Sinha , S. Sirtl , M. Slunecka , J. Smolik , A. Srnka , D. Steffen , M. Stolarski , O. Subrt , M. Sulc , H. Suzuki , A. Szabelski , T. Szameitat , P. Sznajder , M. Tasevsky , S. Tessaro , F. Tessarotto , A. Thiel , J. Tomsa , F. Tosello , V. Tskhay , S. Uhl , B. I. Vasilishin , A. Vauth , B. M. Veit , J. Veloso , A. Vidon , M. Virius , S. Wallner , M. Wilfert , J. ter Wolbeek , K. Zaremba , P. Zavada , M. Zavertyaev , E. Zemlyanichkina , N. Zhuravlev , M. Ziembicki

Recently dispersion relations have been applied to hard exclusive processes such as deeply virtual Compton scattering, and a holographic principle was proposed that maps out the generalized parton distributions entering the soft matrix…

High Energy Physics - Phenomenology · Physics 2009-11-05 Gary R. Goldstein , Simonetta Liuti

A model for deeply virtual Compton scattering, based on analytical light-cone hadron wave functions is presented and studied at energies currently accessible at Jefferson Laboratory, DESY, and beyond. It is shown that perpendicular vector…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. Gardestig , A. P. Szczepaniak , J. T. Londergan

We present our current progress in the holographic computation of the scattering amplitude for Deeply Virtual Compton Scattering (DVCS) processe, as a function of the Mandelstam invariant $t$. We show that it is possible to describe…

High Energy Physics - Phenomenology · Physics 2021-07-07 Artur Amorim , Miguel S. Costa , Robert C. Quevedo

I report on a formalism introduced recently to combine parton shower Monte Carlo's and next-to-leading order QCD computations.

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

Parameter-free and perturbatively stable leading order (LO) and next-to-leading order (NLO) parton densities for real and virtual photons are presented.

High Energy Physics - Phenomenology · Physics 2007-05-23 I. Schienbein

We outline the twist-two analysis of deeply virtual Compton scattering (DVCS)within the conformal partial wave expansion of the amplitude, represented as a Mellin--Barnes integral. The complete next-to-leading order results, including…

High Energy Physics - Phenomenology · Physics 2017-08-23 K. Kumerički , D. Müller , K. Passek-Kumerički

We present a Monte Carlo generator for exclusive vector meson production in charged lepton-proton interactions, l+p --> l+p+V, based on a QCD leading logarithm model calculation according to which the cross section for this process is…

High Energy Physics - Phenomenology · Physics 2009-10-28 M. Arneodo , L. Lamberti , M. Ryskin

We present the implementation within the Pythia8 event generator of a set of parton distributions based on NNPDF methodology. We construct a set of leading-order parton distributions with QED corrections, NNPDF2.3QED LO set, based on the…

High Energy Physics - Phenomenology · Physics 2013-11-26 Stefano Carrazza , Stefano Forte , Juan Rojo

We discuss possibilities of measurement of deeply virtual Compton scattering amplitudes via different asymmetries in order to access the underlying skewed parton distributions. Perturbative one-loop coefficient functions and two-loop…

High Energy Physics - Phenomenology · Physics 2009-10-31 A. V. Belitsky , D. Müller , L. Niedermeier , A. Schäfer

We have developped a fitting code based on the leading-twist handbag Deep Virtual Compton Scattering (DVCS) amplitude in order to extract the Generalized Parton Distributions (GPD) information from DVCS observables in the valence region. In…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Guidal

An interesting breakthrough in understanding the elusive inner content of nuclear systems in terms of partonic degrees of freedom is represented by deeply virtual Compton scattering processes. In such a way, tomographic view of nuclei and…

Nuclear Theory · Physics 2019-10-22 Sara Fucini , Sergio Scopetta , Michele Viviani

The concepts of Generalized Parton Distributions (GPD) are reviewed in an introductory and phenomenological fashion. These distributions provide a rich and unifying picture of the nucleon structure. Their physical meaning is discussed. The…

High Energy Physics - Phenomenology · Physics 2009-11-07 Michel Garcon

The dispersive representation of the virtual Compton forward scattering amplitude has been recently reexamined in connection with the evaluation of the Cottingham formula for the proton-neutron electromagnetic mass difference. The most…

High Energy Physics - Phenomenology · Physics 2016-04-15 Irinel Caprini
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