Measurement Of Deeply Virtual Compton Scattering With A Polarized-Proton Target

Chen S,Avakian H,Burkert V D,Eugenio P,Adams G,Amarian M,Ambrozewicz P,Anghinolfi M,Asryan G,Bagdasaryan H, Baillie N,Ball J P, Baltzell N A, Barrow S, Batourine V,Battaglieri M,Beard K,Bedlinskiy I,Bektasoglu M,Bellis M,Benmouna N, Berman B L,Biselli A S,Bonner B E,Bouchigny S,Boiarinov S,Bosted P,Bradford R, Branford D,Briscoe W J,Brooks W K,Bültmann S,Butuceanu C, Calarco J R, Careccia S L,Carman D S,Carnahan B, Cazes A, Cole P L,Collins P,Coltharp P, Cords D, Corvisiero P, Crabb D,Crannell H,Crede V,Cummings J P,DeMasi R,DeVita R,De Sanctis E,Degtyarenko P V,Denizli H,Dennis L,Deur A,Dharmawardane K V, Dhuga K S,Djalali C,Dodge G E,Donnelly J, Doughty D,Dugger M,Dytman S,Dzyubak O P,Egiyan H,Egiyan K S,El Fassi L,Elouadrhiri L,Fatemi R,Fedotov G,Feldman G,Feuerbach R J,Forest T A,Funsten H,Garçon M,Gavalian G,Gilfoyle G P,Giovanetti K L,Girod F X, Goetz J T,Golovatch E,Gonenc A,Gothe R W,Griffioen K A, Guidal M,Guillo M,Guler N,Guo L,Gyurjyan V, Hadjidakis C,Hafidi K,Hakobyan H,Hakobyan R S,Hardie J,Heddle D,Hersman F W, Hicks K,Hleiqawi I,Holtrop M,Huertas M,Hyde-Wright C E, Ilieva Y,Ireland D G,Ishkhanov B S,Isupov E L,Ito M M,Jenkins D,Jo H S, Joo K,Juengst H G,Keith C,Kellie J D,Khandaker M, Kim K Y, Kim K,Kim W,Klein A, Klein F J,Klusman M, Kossov M,Kramer L H,Kubarovsky V,Kuhn J,Kuhn S E,Kuleshov S V,Lachniet J,Laget J M,Langheinrich J, Lawrence D,Li Ji,Lima A C S,Livingston K,Lu H,Lukashin K,MacCormick M,Markov N,McAleer S,McKinnon B,McNabb J W C, Mecking B A,Mestayer M D,Meyer C A,Mibe T,Mikhailov K,Minehart R, Mirazita M,Miskimen R,Mokeev V,Morand L,Morrow S A,Moteabbed M, Mueller J,Mutchler G S,Nadel-Turonski P,Napolitano J,Nasseripour R,Natasha N,Niccolai S,Niculescu G,Niculescu I,Niczyporuk B B,Niroula M R,Niyazov R A,Nozar M,O'Rielly G V,Osipenko M,Ostrovidov A I, Park K,Pasyuk E,Paterson C,Philips S A,Pierce J,Pivnyuk N,Pocanic D,Pogorelko O,Polli E,Popa I,Pozdniakov S,Preedom B M,Price J W,Prok Y,Protopopescu D,Qin L M,Raue B A,Riccardi G, Ricco G,Ripani M,Ritchie B G,Ronchetti F,Rosner G,Rossi P,Rowntree D,Rubin P D,Sabatié F,Salgado C,Santoro J P,Sapunenko V,Schumacher R A,Serov V S,Sharabian Y G, Shaw J,Shvedunov N V,Skabelin A V,Smith E S,Smith L C, Sober D I,Stavinsky A, Stepanyan S S,Stepanyan S, Stokes B E, Stoler P,Strakovsky I I, Strauch S,Suleiman R,Taiuti M,Tedeschi D J, Thoma U,Tkabladze A,Tkachenko S,Todor L,Tur C,Ungaro M,Vanderhaeghen M,Vineyard M F,Vlassov A V,Watts D P,Weinstein L B,Weygand D P,Williams M, Wolin E,Wood M H,Yegneswaran A, Yun J,Zana L,Zhang J,Zhao B,Zhao Z, Null Null

PHYSICAL REVIEW LETTERS(2006)

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摘要
The longitudinal target-spin asymmetry A(UL) for the exclusive electroproduction of high-energy photons was measured for the first time in ep -> e(')p gamma. The data have been accumulated at JLab with the CLAS spectrometer using 5.7 GeV electrons and a longitudinally polarized NH3 target. A significant azimuthal angular dependence was observed, resulting from the interference of the deeply virtual Compton scattering and Bethe-Heitler processes. The amplitude of the sin phi moment is 0.252 +/- 0.042(stat)+/- 0.020(sys). Theoretical calculations are in good agreement with the magnitude and the kinematic dependence of the target-spin asymmetry, which is sensitive to the generalized parton distributions (H) over tilde and H.
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nuclear theory,electron beam,monte carlo
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