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Exclusive π0 electroproduction at W>2 GeV with clas exclusive π0 electroproduction at W>2 ⋯ I. BEDLINSKIY et al.

  • I. Bedlinskiy
  • , V. Kubarovsky
  • , S. Niccolai
  • , P. Stoler
  • , K. P. Adhikari
  • , M. D. Anderson
  • , S. Anefalos Pereira
  • , H. Avakian
  • , J. Ball
  • , N. A. Baltzell
  • , M. Battaglieri
  • , V. Batourine
  • , A. S. Biselli
  • , S. Boiarinov
  • , J. Bono
  • , W. J. Briscoe
  • , W. K. Brooks
  • , V. D. Burkert
  • , D. S. Carman
  • , A. Celentano
  • S. Chandavar, L. Colaneri, P. L. Cole, M. Contalbrigo, O. Cortes, V. Crede, A. D'Angelo, N. Dashyan, R. De Vita, E. De Sanctis, A. Deur, C. Djalali, D. Doughty, R. Dupre, H. Egiyan, A. El Alaoui, L. El Fassi, L. Elouadrhiri, P. Eugenio, G. Fedotov, S. Fegan, J. A. Fleming, T. A. Forest, B. Garillon, M. Garçon, G. Gavalian, N. Gevorgyan, Y. Ghandilyan, G. P. Gilfoyle, K. L. Giovanetti, F. X. Girod, E. Golovatch, R. W. Gothe, K. A. Griffioen, B. Guegan, L. Guo, K. Hafidi, H. Hakobyan, N. Harrison, M. Hattawy, K. Hicks, M. Holtrop, D. G. Ireland, B. S. Ishkhanov, E. L. Isupov, D. Jenkins, H. S. Jo, K. Joo, D. Keller, M. Khandaker, A. Kim, W. Kim, A. Klein, F. J. Klein, S. Koirala, S. E. Kuhn, S. V. Kuleshov, P. Lenisa, W. I. Levine, K. Livingston, H. Y. Lu, I. J.D. Macgregor, N. Markov, M. Mayer, B. McKinnon, M. Mirazita, V. Mokeev, R. A. Montgomery, C. I. Moody, H. Moutarde, A. Movsisyan, C. Munoz Camacho, P. Nadel-Turonski, I. Niculescu, M. Osipenko, A. I. Ostrovidov, L. L. Pappalardo, K. Park, S. Park, E. Pasyuk, E. Phelps, W. Phelps, J. J. Phillips, S. Pisano, O. Pogorelko, J. W. Price, Y. Prok, D. Protopopescu, S. Procureur, A. J.R. Puckett, B. A. Raue, M. Ripani, B. G. Ritchie, A. Rizzo, P. Rossi, P. Roy, F. Sabatié, C. Salgado, D. Schott, R. A. Schumacher, E. Seder, I. Senderovich, Y. G. Sharabian, A. Simonyan, G. D. Smith, D. I. Sober, D. Sokhan, S. S. Stepanyan, S. Strauch, V. Sytnik, W. Tang, Ye Tian, M. Ungaro, A. V. Vlassov, H. Voskanyan, E. Voutier, N. K. Walford, D. Watts, X. Wei, L. B. Weinstein, M. Yurov, N. Zachariou, L. Zana, J. Zhang, Z. W. Zhao, I. Zonta
  • Alikhanov Institute for Theoretical and Experimental Physics
  • Rensselaer Polytechnic Institute
  • Thomas Jefferson National Accelerator Facility
  • George Washington University
  • Institut de Physique Nucléaire Orsay
  • Old Dominion University
  • University of Glasgow
  • National Institute for Nuclear Physics
  • CEA Saclay
  • Argonne National Laboratory
  • University of South Carolina
  • Kyungpook National University
  • Fairfield University
  • Florida International University
  • Universidad Técnica Federico Santa Maria
  • Ohio University
  • Idaho State University
  • Florida State University
  • University of Rome Tor Vergata
  • A. Alikhanian Yerevan Institute of Physics
  • Christopher Newport University
  • University of New Hampshire
  • Lomonosov Moscow State University
  • University of Edinburgh
  • University of Richmond
  • James Madison University
  • College of William and Mary
  • University of Connecticut
  • Virginia Polytechnic Institute and State University
  • University of Virginia
  • Norfolk State University
  • Catholic University of America
  • Carnegie Mellon University
  • California State University Dominguez Hills
  • Arizona State University
  • Université Joseph Fourier Grenoble 1

Research output: Contribution to journalArticlepeer-review

49 Scopus citations

Abstract

Exclusive neutral-pion electroproduction (ep→e′p′π0) was measured at Jefferson Lab with a 5.75-GeV electron beam and the CLAS detector. Differential cross sections d4σ/dtdQ2dxBdφπ and structure functions σT+εσL,σTT, and σLT as functions of t were obtained over a wide range of Q2 and xB. The data are compared with Regge and handbag theoretical calculations. Analyses in both frameworks find that a large dominance of transverse processes is necessary to explain the experimental results. For the Regge analysis it is found that the inclusion of vector meson rescattering processes is necessary to bring the magnitude of the calculated and measured structure functions into rough agreement. In the handbag framework, there are two independent calculations, both of which appear to roughly explain the magnitude of the structure functions in terms of transversity generalized parton distributions.

Original languageEnglish
Article number025205
JournalPhysical Review C - Nuclear Physics
Volume90
Issue number2
DOIs
StatePublished - 13 Aug 2014

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