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Induced polarization of Λ(1116) in kaon electroproduction

  • M. Gabrielyan
  • , B. A. Raue
  • , D. S. Carman
  • , K. Park
  • , K. P. Adhikari
  • , D. Adikaram
  • , M. J. Amaryan
  • , S. Anefalos Pereira
  • , H. Avakian
  • , J. Ball
  • , N. A. Baltzell
  • , M. Battaglieri
  • , V. Baturin
  • , I. Bedlinskiy
  • , A. S. Biselli
  • , J. Bono
  • , S. Boiarinov
  • , W. J. Briscoe
  • , W. K. Brooks
  • , V. D. Burkert
  • T. Cao, A. Celentano, S. Chandavar, G. Charles, 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, L. El Fassi, P. Eugenio, G. Fedotov, S. Fegan, J. A. Fleming, T. A. Forest, B. Garillon, N. Gevorgyan, Y. Ghandilyan, G. P. Gilfoyle, K. L. Giovanetti, F. X. Girod, J. T. Goetz, E. Golovatch, R. W. Gothe, K. A. Griffioen, M. Guidal, L. Guo, K. Hafidi, H. Hakobyan, M. Hattawy, K. Hicks, D. Ho, M. Holtrop, S. M. Hughes, Y. Ilieva, D. G. Ireland, B. S. Ishkhanov, D. Jenkins, H. Jiang, H. S. Jo, K. Joo, D. Keller, M. Khandaker, W. Kim, F. J. Klein, S. Koirala, V. Kubarovsky, S. E. Kuhn, S. V. Kuleshov, P. Lenisa, W. I. Levine, K. Livingston, I. J.D. Macgregor, M. Mayer, B. McKinnon, C. A. Meyer, M. D. Mestayer, M. Mirazita, V. Mokeev, C. I. Moody, H. Moutarde, A. Movsisyan, E. Munevar, C. Munoz Camacho, P. Nadel-Turonski, S. Niccolai, G. Niculescu, M. Osipenko, L. L. Pappalardo, R. Paremuzyan, E. Pasyuk, P. Peng, W. Phelps, J. J. Phillips, S. Pisano, O. Pogorelko, S. Pozdniakov, J. W. Price, S. Procureur, D. Protopopescu, D. Rimal, M. Ripani, A. Rizzo, F. Sabatié, C. Salgado, D. Schott, R. A. Schumacher, A. Simonyan, G. D. Smith, D. I. Sober, D. Sokhan, S. S. Stepanyan, S. Stepanyan, I. I. Strakovsky, S. Strauch, V. Sytnik, W. Tang, M. Ungaro, A. V. Vlassov, H. Voskanyan, E. Voutier, N. K. Walford, D. P. Watts, X. Wei, L. B. Weinstein, N. Zachariou, L. Zana, J. Zhang, I. Zonta
  • Florida International University
  • Thomas Jefferson National Accelerator Facility
  • Kyungpook National University
  • Old Dominion University
  • National Institute for Nuclear Physics
  • CEA Saclay
  • Argonne National Laboratory
  • Arizona State University
  • Alikhanov Institute for Theoretical and Experimental Physics
  • Carnegie Mellon University
  • Fairfield University
  • George Washington University
  • Universidad Técnica Federico Santa Maria
  • University of South Carolina
  • Ohio University
  • Institut de Physique Nucléaire Orsay
  • Idaho State University
  • Florida State University
  • A. Alikhanian Yerevan Institute of Physics
  • Christopher Newport University
  • Lomonosov Moscow State University
  • University of Edinburgh
  • University of Richmond
  • James Madison University
  • College of William and Mary
  • University of New Hampshire
  • University of Glasgow
  • Virginia Polytechnic Institute and State University
  • University of Connecticut
  • University of Virginia
  • Norfolk State University
  • Catholic University of America
  • Rensselaer Polytechnic Institute
  • California State University Dominguez Hills
  • Université Joseph Fourier Grenoble 1

Research output: Contribution to journal › Article › peer-review

17 Scopus citations

Abstract

We have measured. the induced polarization of the Λ(1116) in the reaction ep→e′K+Λ, detecting the scattered e′ and K+ in the final state along with the proton from the decay Λ→pπ-. The present study used the CEBAF Large Acceptance Spectrometer (CLAS), which allowed for a large kinematic acceptance in invariant energy W (1.6≤W≤2.7 GeV) and covered the full range of the kaon production angle at an average momentum transfer Q2=1.90GeV2. In this experiment a 5.50-GeV electron beam was incident upon an unpolarized liquid-hydrogen target. We have mapped out the W and kaon production angle dependencies of the induced polarization and found striking differences from photoproduction data over most of the kinematic range studied. However, we also found that the induced polarization is essentially Q2 independent in our kinematic domain, suggesting that somewhere below the Q2 covered here there must be a strong Q2 dependence. Along with previously published photo- and electroproduction cross sections and polarization observables, these data are needed for the development of models, such as effective field theories, and as input to coupled-channel analyses that can provide evidence of previously unobserved s-channel resonances.

Original languageEnglish
Article number035202
JournalPhysical Review C - Nuclear Physics
Volume90
Issue number3
DOIs
StatePublished - 15 Sep 2014

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