Precision measurements of g1 of the proton and of the deuteron with 6 GeV electrons

Y Prok,Peter Bosted,N D Kvaltine,K P Adhikari,D Adikaram,M Aghasyan,M J Amaryan,Michael Anderson,S Anefalos Pereira,H Avakian,H Baghdasaryan, James P Ball,N A Baltzell,M Battaglieri,A S Biselli,Johann S De Bono,W J Briscoe, Jean C Brock, W K Brooks,S Bultmann,V D Burkert,Cathleen Carlin,D S Carman,A Celentano,S Chandavar,L Colaneri,P L Cole,M Contalbrigo,O Cortes,D Crabb,V Crede,A Dangelo,N Dashyan,R De Vita,E De Sanctis,A Deur,C Djalali,G E Dodge,D Doughty,R Dupre,A El Alaoui,L El Fassi,L Elouadrhiri,G Fedotov,S J Fegan,R G Fersch,J A Fleming,T A Forest,M Garcon,B Garillon,N Gevorgyan,Y Ghandilyan,G P Gilfoyle,F X Girod, K L Giovanetti,J T Goetz,W Gohn,R W Gothe,K A Griffioen, B Guegan,N Guler,K Hafidi,C Hanretty, N M Harrison,M Hattawy,K Hicks,D Ho,M Holtrop,Y Ilieva,D G Ireland,B S Ishkhanov,E L Isupov,S S Jawalkar, Xunfei Jiang,H S Jo,K Joo,N Kalantarians,C D Keith,D Keller,M Khandaker,A Kim, W Kim,A Klein,F J Klein,S Koirala,V Kubarovsky,S E Kuhn,S Kuleshov,P Lenisa, K Livingston,H Y Lu,I J D Macgregor,N Markov,M Mayer,B Mckinnon,D Meekins,T Mineeva,M Mirazita,V Mokeev, R A Montgomery,H Moutarde,A Movsisyan,E Munevar,C Munoz Camacho,P Nadelturonski,S Niccolai,G Niculescu,I Niculescu,M Osipenko,A I Ostrovidov,L L Pappalardo,R Paremuzyan,K Park, Pai Peng, J J Phillips,Jacalyn H Pierce,S Pisano,O Pogorelko,S Pozdniakov,J W Price,S Procureur,D Protopopescu,A J R Puckett,B A Raue,D Rimal,M Ripani, A Rizzo,G Rosner,P Rossi,P Roy,F Sabatie,M S Saini,C Salgado,D Schott,R A Schumacher,E Seder,Y G Sharabian,A Simonyan,C M Smith,George Davey Smith,D I Sober,D Sokhan,S S Stepanyan,I I Strakovsky,S Strauch,V Sytnik,M Taiuti,Wansheng Tang,S Tkachenko,M Ungaro,B Vernarsky,A V Vlassov,H Voskanyan,E Voutier,N K Walford,D P Watts,L B Weinstein,N Zachariou,L Zana,Jinzhong Zhang,Baoxiang Zhao,Z W Zhao,I Zonta

PHYSICAL REVIEW C(2014)

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摘要
The inclusive polarized structure functions of the proton and deuteron, g(1)(p) and g(1)(d) , were measured with high statistical precision using polarized 6 GeV electrons incident on a polarized ammonia target in Hall B at Jefferson Laboratory. Electrons scattered at laboratory angles between 18 and 45 degrees were detected using the CEBAF Large Acceptance Spectrometer (CLAS). For the usual deep inelastic region kinematics, Q(2) > 1 GeV2 and the final-state invariant mass W > 2 GeV, the ratio of polarized to unpolarized structure functions g(1)/F-1 is found to be nearly independent of Q(2) at fixed x. Significant resonant structure is apparent at values of W up to 2.3 GeV. In the framework of perturbative quantum chromodynamics, the high-W results can be used to better constrain the polarization of quarks and gluons in the nucleon, as well as high-twist contributions.
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