Measurement of semi-inclusive π+ electroproduction off the proton

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

PHYSICAL REVIEW D(2009)

引用 82|浏览136
暂无评分
摘要
Semi-inclusive pi(+) electroproduction on protons has been measured with the CLAS detector at Jefferson Lab. The measurement was performed on a liquid-hydrogen target using a 5.75 GeV electron beam. The complete five-fold differential cross sections were measured over a wide kinematic range including the complete range of azimuthal angles between hadronic and leptonic planes, phi, enabling us to separate the phi-dependent terms. Our measurements of the phi-independent term of the cross section at low Bjorken x were found to be in fairly good agreement with pQCD calculations. Indeed, the conventional current fragmentation calculation can account for almost all of the observed cross section, even at small pi(+) momentum. The measured center-of-momentum spectra are in qualitative agreement with high-energy data, which suggests a surprising numerical similarity between the spectator diquark fragmentation in the present reaction and the antiquark fragmentation measured in e(+)e(-) collisions. We have observed that the two phi-dependent terms of the cross section are small. Within our precision the cos2 phi term is compatible with zero, except for the low-z region, and the measured cos phi term is much smaller in magnitude than the sum of the Cahn and Berger effects.
更多
查看译文
AI 理解论文
溯源树
样例
生成溯源树,研究论文发展脉络
Chat Paper
正在生成论文摘要