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    Role of the πN P11 interaction in πd elastic scattering at 50 MeV

    N. R. Stevenson, R. B. Schubank, Y. M. Shin, P. Amaudruz, P. P. J. Delheij, D. C. Healey, B. K. Jennings, D. F. Ottewell, G. Sheffer et al.

    G. R. Smith, G. D. Wait, J. T. Brack, A. Feltham, M. Hanna, R. R. Johnson, F. M. Rozon, V. Sossi, D. Vetterli, P. Weber, N. Grion, R. Rui, M. Kohler, R. A. Ristinen, E. L. Mathie, R. Tacik, M. Yeomans, C. A. Gossett, and G. J. Wagner

    • Department of Physics, University of Saskatchewan, Saskatoon, Saskatchewan, Canada S7N 0W0
    • TRIUMF, 4004 Wesbrook Mall, Vancouver, British Columbia, Canada V6T 2A3
    • Department of Physics, University of British Columbia, Vancouver, British Columbia V6T 1W5
    • Istituto Nazionale di Fisica Nucleare and Dipartimento di Fisica, Università di Trieste, Trieste, Italy 34127
    • Department of Physics, University of Colorado, Boulder, Colorado 80309
    • Department of Physics, University of Regina, Regina, Saskatchewan, Canada S4S 0A2
    • Nuclear Physics Laboratory, Department of Physics, University of Washington, Seattle, Washington 98195
    • Physikalisches Institut der Universitaet Tuebingen, Morgenstelle, D-7400 Tuebingen, Federal Republic of Germany

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    Phys. Rev. Lett. 65, 1987 – Published 15 October, 1990

    DOI: https://doi.org/10.1103/PhysRevLett.65.1987

    Abstract

    Measurements of the vector analyzing power iT11 in π+d elastic scattering at 50 MeV have been made at pion laboratory scattering angles between 60° and 130° using a dynamically polarized target and a magnetic spectrometer. In contrast to measurements of spin observables at higher energies, we find agreement with models that include the πN P11 amplitude and disagreement with models that exclude or suppress it.

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    Phys. Rev. Lett. 65, 1987– Published 15 October, 1990
    • Received 6 July 1990

    © 1990 American Physical Society

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