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Recent results from the Deeply Virtual Compton Scattering (DVCS) program at Jefferson Lab will be presented. Approved dedicated DVCS experiments at 6 GeV and plans for the 12 GeV upgrade will be discussed.

High Energy Physics - Phenomenology · Physics 2014-11-17 Latifa Elouadrhiri

This paper focuses on a measurement of deeply virtual Compton scattering (DVCS) performed at Jefferson Lab using a nearly-6-GeV polarized electron beam, two longitudinally polarized (via DNP) solid targets of protons (NH3) and deuterons…

Nuclear Experiment · Physics 2019-08-13 Silvia Niccolai

In this talk I address two high impact physics programs that require the use of polarized and unpolarized positron beams in addition to using electron beams of the same energy. First, I address what will be gained from using positron beams…

Nuclear Experiment · Physics 2018-06-13 Volker D. Burkert

An overview is given about the capabilities provided by the JLab 12 GeV Upgrade to measure deeply virtual exclusive processes with high statistics and covering a large kinematics range in the parameters that are needed to allow…

High Energy Physics - Phenomenology · Physics 2017-08-23 Latifa Elouadrhiri

In this prize talk, I recall some of the history surrounding the discovery of deeply virtual Compton scattering, and explain why it is an exciting experimental tool to obtain novel tomographic pictures of the nucleons at Jefferson Lab 12…

High Energy Physics - Phenomenology · Physics 2016-05-05 Xiangdong Ji

Measuring Deeply Virtual Compton Scattering on the neutron is one of the necessary steps to understand the structure of the nucleon in terms of Generalized Parton Distributions (GPDs). Neutron targets play a complementary role to…

High Energy Physics - Experiment · Physics 2024-06-26 CLAS Collaboration , A. Hobart , S. Niccolai , M. Čuić , K. Kumerički , P. Achenbach , J. S. Alvarado , W. R. Armstrong , H. Atac , H. Avakian , L. Baashen , N. A. Baltzell , L. Barion , M. Bashkanov , M. Battaglieri , B. Benkel , F. Benmokhtar , A. Bianconi , A. S. Biselli , S. Boiarinov , M. Bondi , W. A. Booth , F. Bossù , K. -Th. Brinkmann , W. J. Briscoe , W. K. Brooks , S. Bueltmann , V. D. Burkert , T. Cao , R. Capobianco , D. S. Carman , P. Chatagnon , G. Ciullo , P. L. Cole , M. Contalbrigo , A. D'Angelo , N. Dashyan , R. De Vita , M. Defurne , A. Deur , S. Diehl , C. Dilks , C. Djalali , R. Dupre , H. Egiyan , A. El Alaoui , L. El Fassi , L. Elouadrhiri , S. Fegan , A. Filippi , C. Fogler , K. Gates , G. Gavalian , G. P. Gilfoyle , D. Glazier , R. W. Gothe , Y. Gotra , M. Guidal , K. Hafidi , H. Hakobyan , M. Hattawy , F. Hauenstein , D. Heddle , M. Holtrop , Y. Ilieva , D. G. Ireland , E. L. Isupov , H. Jiang , H. S. Jo , K. Joo , T. Kageya , A. Kim , W. Kim , V. Klimenko , A. Kripko , V. Kubarovsky , S. E. Kuhn , L. Lanza , M. Leali , S. Lee , P. Lenisa , X. Li , I. J. D. MacGregor , D. Marchand , V. Mascagna , M. Maynes , B. McKinnon , Z. E. Meziani , S. Migliorati , R. G. Milner , T. Mineeva , M. Mirazita , V. Mokeev , C. Muñoz Camacho , P. Nadel-Turonski , P. Naidoo , K. Neupane , G. Niculescu , M. Osipenko , P. Pandey , M. Paolone , L. L. Pappalardo , R. Paremuzyan , E. Pasyuk , S. J. Paul , W. Phelps , N. Pilleux , M. Pokhrel , S. Polcher Rafael , J. Poudel , J. W. Price , Y. Prok , T. Reed , J. Richards , M. Ripani , J. Ritman , P. Rossi , A. A. Golubenko , C. Salgado , S. Schadmand , A. Schmidt , Marshall B. C. Scott , E. M. Seroka , Y. G. Sharabian , E. V. Shirokov , U. Shrestha , N. Sparveris , M. Spreafico , S. Stepanyan , I. I. Strakovsky , S. Strauch , J. A. Tan , N. Trotta , R. Tyson , M. Ungaro , S. Vallarino , L. Venturelli , V. Tommaso , H. Voskanyan , E. Voutier , D. P Watts , X. Wei , R. Williams , M. H. Wood , L. Xu , N. Zachariou , J. Zhang , Z. W. Zhao , M. Zurek

Positron beams, both polarized and unpolarized, are identified as essential ingredients for the experimental program at the next generation of lepton accelerators. In the context of the Hadronic Physics program at the Jefferson Laboratory…

Nuclear Experiment · Physics 2019-06-25 A. Afanasev , I. Albayrak , S. Ali , M. Amaryan , A. D'Angelo , J. Annand , J. Arrington , A. Asaturyan , H. Avakian , T. Averett , L. Barion , M. Battaglieri , V. Bellini , V. Berdnikov , J. Bernauer , A. Biselli , M. Boer , M. Bondì , K. -T. Brinkmann , B. Briscoe , V. Burkert , A. Camsonne , T. Cao , L. Cardman , M. Carmignotto , L. Causse , A. Celentano , P. Chatagnon , G. Ciullo , M. Contalbrigo , D. Day , M. Defurne , S. Diehl , B. Dongwi , R. Dupré , D. Dutta , M. Ehrhart , L. Elouadrhiri , R. Ent , I. Fernando , A. Filippi , Y. Furletova , H. Gao , A. Gasparian , D. Gaskell , F. Georges , F. -X. Girod , J. Grames , C. Gu , M. Guidal , D. Hamilton , D. Hasell , D. Higinbotham , M. Hoballah , T. Horn , C. Hyde , A. Italiano , N. Kalantarians , G. Kalicy , D. Keller , C. Keppel , M. Kerver , P. King , E. Kinney , H. -S. Ko , M. Kohl , V. Kubarovsky , L. Lanza , P. Lenisa , N. Liyanage , S. Liuti , J. Mamei , D. Marchand , P. Markowitz , L. Marsicano , M. Mazouz , M. McCaughan , B. McKinnon , M. Mihovilovič , R. Milner , A. Mkrtchyan , H. Mkrtchyan , A. Movsisyan , C. Muñoz Camacho , P. Nadel-Turońs , M. De Napoli , J. Nazeer , S. Niccolai , G. Niculescu , R. Novotny , L. Pappalardo , R. Paremuzyan , E. Pasyuk , T. Patel , I. Pegg , D. Perera , A. Puckett , N. Randazzo , M. Rashad , M. Rathnayake , A. Rizzo , J. Roche , O. Rondon , A. Schmidt , M. Shabestari , Y. Sharabian , S. Širca , D. Sokhan , A. Somov , N. Sparveris , S. Stepanyan , I. Strakovsky , V. Tadevosyan , M. Tiefenback , R. Trotta , R. De Vita , H. Voskanyan , E. Voutier , R. Wang , B. Wojtsekhowski , S. Wood , H. -G. Zaunick , S. Zhamkochyan , J. Zhang , S. Zhao , X. Zheng , C. Zorn

Positron initiated deeply virtual Compton scattering (DVCS) off $^4$He and $^3$He nuclei is described. The way the so-called $d-$term could be obtained from the real part of the relevant Compton form factor is summarized, and the importance…

High Energy Physics - Phenomenology · Physics 2021-09-29 Sara Fucini , Mohammad Hattawy , Matteo Rinaldi , Sergio Scopetta

The Virtual Compton scattering (VCS) process at low energies explores the electromagnetic structure of the proton in terms of generalized polarizabilities (GPs). In the one-photon exchange approximation, VCS can be accessed with exclusive…

High Energy Physics - Phenomenology · Physics 2021-12-08 B. Pasquini , M. Vanderhaeghen

In the context of nucleon structure studies, Generalized Parton Distributions (GPDs) are crucial for understanding the correlation between the longitudinal momentum and the transverse position of partons inside the nucleon. A privileged…

High Energy Physics - Experiment · Physics 2025-09-16 J. S. Alvarado , M. Hoballah , E. Voutier

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 and DESY. It is shown that poles and perpendicular vector…

High Energy Physics - Phenomenology · Physics 2017-08-23 A. Gardestig , A. P. Szczepaniak , J. T. Londergan

Double deeply virtual Compton scattering (DDVCS) is a very precise tool for the nucleon tomography. Its measurement requires high luminosity electron beams and precise dedicated detectors, since its amplitude is quite small in the…

High Energy Physics - Phenomenology · Physics 2024-01-25 K. Deja , V. Martinez-Fernandez , B. Pire , P. Sznajder , J. Wagner

Deeply virtual Compton scattering (DVCS) is the golden exclusive channel for the study of the partonic structure of hadrons, within the universal framework of generalized parton distributions (GPDs). This paper presents the aim and general…

Nuclear Experiment · Physics 2008-09-24 Eric Voutier

The beam charge asymmetry helps to isolate the real part of the deeply virtual Compton scattering (DVCS) amplitude. It is discussed what information can be gained both from the real and imaginary part of the DVCS amplitude.

High Energy Physics - Phenomenology · Physics 2015-05-13 Matthias Burkardt

We present the recent data issued from the Halls A and B of Jefferson Laboratory for the Deep Virtual Compton Scattering Process on the proton. An important set of data for beam spin asymmetries, unpolarized cross sections and differences…

High Energy Physics - Phenomenology · Physics 2008-12-18 M. Guidal

A major part of the future COMPASS program is dedicated to the investigation of the nucleon structure through Deeply Virtual Compton Scattering (DVCS) and Deeply Virtual Meson Production (DVMP). COMPASS will measure DVCS and DVMP reactions…

High Energy Physics - Experiment · Physics 2020-01-09 A. Ferrero

Positron beams, both polarized and unpolarized, are identified as essential ingredients for the experimental programs at the next generation of lepton accelerators. In the context of the hadronic physics program at Jefferson Lab (JLab),…

Nuclear Experiment · Physics 2021-09-15 A. Accardi , A. Afanasev , I. Albayrak , S. F. Ali , M. Amaryan , J. R. M. Annand , J. Arrington , A. Asaturyan , H. Atac , H. Avakian , T. Averett , C. Ayerbe Gayoso , X. Bai , L. Barion , M. Battaglieri , V. Bellini , R. Beminiwattha , F. Benmokhtar , V. V. Berdnikov , J. C. Bernauer , V. Bertone , A. Bianconi , A. Biselli , P. Bisio , P. Blunden , M. Boer , M. Bondì , K. -T. Brinkmann , W. J. Briscoe , V. Burkert , T. Cao , A. Camsonne , R. Capobianco , L. Cardman , M. Carmignotto , M. Caudron , L. Causse , A. Celentano , P. Chatagnon , J. -P. Chen , T. Chetry , G. Ciullo , E. Cline , P. L. Cole , M. Contalbrigo , G. Costantini , A. D'Angelo , L. Darmé , D. Day , M. Defurne , M. De Napoli , A. Deur , R. De Vita , N. D'Hose , S. Diehl , M. Diefenthaler , B. Dongwi , R. Dupré , H. Dutrieux , D. Dutta , M. Ehrhart , L. El Fassi , L. Elouadrhiri , R. Ent , J. Erler , I. P. Fernando , A. Filippi , D. Flay , T. Forest , E. Fuchey , S. Fucini , Y. Furletova , H. Gao , D. Gaskell , A. Gasparian , T. Gautam , F. -X. Girod , K. Gnanvo , J. Grames , G. N. Grauvoge , P. Gueye , M. Guidal , S. Habet , T. J. Hague , D. J. Hamilton , O. Hansen , D. Hasell , M. Hattawy , D. W. Higinbotham , A. Hobart , T. Horn , C. E. Hyde , H. Ibrahim , A. Ilyichev , A. Italiano , K. Joo , S. J. Joosten , V. Khachatryan , N. Kalantarians , G. Kalicy , B. Karky , D. Keller , C. Keppel , M. Kerver , M. Khandaker , A. Kim , J. Kim , P. M. King , E. Kinney , V. Klimenko , H. -S. Ko , M. Kohl , V. Kozhuharov , B. T. Kriesten , G. Krnjaic , V. Kubarovsky , T. Kutz , L. Lanza , M. Leali , P. Lenisa , N. Liyanage , Q. Liu , S. Liuti , J. Mammei , S. Mantry , D. Marchand , P. Markowitz , L. Marsicano , V. Mascagna , M. Mazouz , M. McCaughan , B. McKinnon , D. McNulty , W. Melnitchouk , A. Metz , Z. -E. Meziani , S. Migliorati , M. Mihovilovic , R. Milner , A. Mkrtchyan , H. Mkrtchyan , A. Movsisyan , H. Moutarde , M. Muhoza , C. Muñoz Camacho , J. Murphy , P. Nadel-Turonski , E. Nardi , J. Nazeer , S. Niccolai , G. Niculescu , R. Novotny , J. F. Owens , M. Paolone , L. Pappalardo , R. Paremuzyan , B. Pasquini , E. Pasyuk , T. Patel , I. Pegg , C. Peng , D. Perera , M. Poelker , K. Price , A. J. R. Puckett , M. Raggi , N. Randazzo , M. N. H. Rashad , M. Rathnayake , B. Raue , P. E. Reimer , M. Rinaldi , A. Rizzo , Y. Roblin , J. Roche , O. Rondon-Aramayo , F. Sabatié , G. Salmè , E. Santopinto , R. Santos Estrada , B. Sawatzky , A. Schmidt , P. Schweitzer , S. Scopetta , V. Sergeyeva , M. Shabestari , A. Shahinyan , Y. Sharabian , S. Širca , E. S. Smith , D. Sokhan , A. Somov , N. Sparveris , M. Spata , H. Spiesberger , M. Spreafico , S. Stepanyan , P. Stoler , I. Strakovsky , R. Suleiman , M. Suresh , P. Sznajder , H. Szumila-Vance , V. Tadevosyan , A. S. Tadepalli , A. W. Thomas , M. Tiefenback , R. Trotta , M. Ungaro , P. Valente , M. Vanderhaeghen , L. Venturelli , H. Voskanyan , E. Voutier , B. Wojtsekhowski , M. H. Wood , S. Wood , J. Xie , W. Xiong , Z. Ye , M. Yurov , H. -G. Zaunick , S. Zhamkochyan , J. Zhang , S. Zhang , S. Zhao , Z. W. Zhao , X. Zheng , J. Zhou , C. Zorn

We study deeply virtual Compton scattering (DVCS) on a deuteron target. We model the Generalized Quark Distributions in the deuteron by using the impulse approximation for the lowest Fock-space state. Numerical predictions are given for the…

High Energy Physics - Phenomenology · Physics 2009-11-07 F. Cano , B. Pire

Generalized Parton Distributions (GPDs) are multidimensional structure functions of hadrons, encoding mechanical and spin properties through the correlation of the momentum and transverse position of partons. While channels like Deeply…

High Energy Physics - Phenomenology · Physics 2025-09-16 J. S. Alvarado , M. Hoballah , E. Voutier
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