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Measurement of the generalized form factors near threshold via γ*p→nπ+ at high Q2

  • K. Park
  • , R. W. Gothe
  • , K. P. Adhikari
  • , D. Adikaram
  • , M. Anghinolfi
  • , H. Baghdasaryan
  • , J. Ball
  • , M. Battaglieri
  • , V. Batourine
  • , I. Bedlinskiy
  • , R. P. Bennett
  • , A. S. Biselli
  • , C. Bookwalter
  • , S. Boiarinov
  • , D. Branford
  • , W. J. Briscoe
  • , W. K. Brooks
  • , V. D. Burkert
  • , D. S. Carman
  • , A. Celentano
  • S. Chandavar, G. Charles, P. L. Cole, M. Contalbrigo, V. Crede, A. D'Angelo, A. Daniel, N. Dashyan, R. De Vita, E. De Sanctis, A. Deur, C. Djalali, D. Doughty, R. Dupre, A. El Alaoui, L. El Fassi, P. Eugenio, G. Fedotov, A. Fradi, M. Y. Gabrielyan, N. Gevorgyan, G. P. Gilfoyle, K. L. Giovanetti, F. X. Girod, J. T. Goetz, W. Gohn, E. Golovatch, L. Graham, K. A. Griffioen, M. Guidal, L. Guo, K. Hafidi, H. Hakobyan, C. Hanretty, D. Heddle, K. Hicks, M. Holtrop, C. E. Hyde, Y. Ilieva, D. G. Ireland, B. S. Ishkhanov, E. L. Isupov, D. Jenkins, H. S. Jo, K. Joo, N. Kalantarians, M. Khandaker, P. Khetarpal, A. Kim, W. Kim, A. Klein, F. J. Klein, A. Kubarovsky, V. Kubarovsky, S. E. Kuhn, S. V. Kuleshov, N. D. Kvaltine, K. Livingston, H. Y. Lu, I. J.D. MacGregor, N. Markov, M. Mayer, B. McKinnon, M. D. Mestayer, C. A. Meyer, T. Mineeva, M. Mirazita, V. Mokeev, H. Moutarde, E. Munevar, P. Nadel-Turonski, R. Nasseripour, S. Niccolai, G. Niculescu, I. Niculescu, M. Osipenko, A. I. Ostrovidov, M. Paolone, L. Pappalardo, R. Paremuzyan, S. Park, S. Anefalos Pereira, E. Phelps, S. Pisano, O. Pogorelko, S. Pozdniakov, J. W. Price, S. Procureur, Y. Prok, G. Ricco, D. Rimal, M. Ripani, B. G. Ritchie, G. Rosner, P. Rossi, F. Sabatié, M. S. Saini, C. Salgado, D. Schott, R. A. Schumacher, H. Seraydaryan, Y. G. Sharabian, E. S. Smith, G. D. Smith, D. I. Sober, D. Sokhan, S. S. Stepanyan, S. Stepanyan, P. Stoler, I. I. Strakovsky, S. Strauch, M. Taiuti, W. Tang, C. E. Taylor, Y. Tian, S. Tkachenko, A. Trivedi, M. Ungaro, B. Vernarsky, A. V. Vlassov, E. Voutier, D. P. Watts, D. P. Weygand, M. H. Wood, N. Zachariou, B. Zhao, Z. W. Zhao
  • University of South Carolina
  • Thomas Jefferson National Accelerator Facility
  • Old Dominion University
  • National Institute for Nuclear Physics
  • University of Virginia
  • A. Alikhanian Yerevan Institute of Physics
  • CEA Saclay
  • Alikhanov Institute for Theoretical and Experimental Physics
  • Fairfield University
  • Rensselaer Polytechnic Institute
  • Florida State University
  • University of Edinburgh
  • George Washington University
  • Universidad Técnica Federico Santa Maria
  • Ohio University
  • Idaho State University
  • University of Rome Tor Vergata
  • Christopher Newport University
  • Argonne National Laboratory
  • Institut de Physique Nucléaire Orsay
  • Florida International University
  • University of Richmond
  • James Madison University
  • University of California at Los Angeles
  • University of Connecticut
  • Lomonosov Moscow State University
  • College of William and Mary
  • University of New Hampshire
  • University of Glasgow
  • Virginia Polytechnic Institute and State University
  • Norfolk State University
  • Kyungpook National University
  • Catholic University of America
  • Carnegie Mellon University
  • California State University Dominguez Hills
  • University of Genoa
  • Arizona State University
  • Université Joseph Fourier Grenoble 1
  • Canisius College

Research output: Contribution to journalArticlepeer-review

21 Scopus citations

Abstract

We report the first extraction of the pion-nucleon multipoles near the production threshold for the nπ+ channel at relatively high momentum transfer (Q2 up to 4.2 GeV2). The dominance of the s-wave transverse multipole (E0+), expected in this region, allowed us to access the generalized form factor G1 within the light-cone sum-rule (LCSR) framework as well as the axial form factor GA. The data analyzed in this work were collected by the nearly 4π CEBAF Large Acceptance Spectrometer (CLAS) using a 5.754-GeV electron beam on a proton target. The differential cross section and the π-N multipole E0+/GD were measured using two different methods, the LCSR and a direct multipole fit. The results from the two methods are found to be consistent and almost Q2 independent.

Original languageEnglish
Article number035208
JournalPhysical Review C - Nuclear Physics
Volume85
Issue number3
DOIs
StatePublished - 26 Mar 2012

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