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  • Pospischil, Th; Bartsch, P; Baumann, D; Bermuth, J; Boehm, R; Bohinc, K; Derber, S; Ding, M; Distler, M; Drechsel, D; Elsner, D; Ewald, I; Friedrich, J; Friedrich, J M; Geiges, R; Hedicke, S; Jennewein, P; Kahrau, M; Kamalov, S S; Klein, F; Krygier, K W; Lac, J; Liesenfeld, A; McIntyre, J; Merkel, H; Merle, P; Mueller, U; Neuhausen, R; Potokar, M; Ransome, R D; Rohe, D; Rosner, G; Schmieden, H; Seimetz, M; Sirca, S; Sick, I; Suele, A; Tiator, L; Wagner, A; Walcher, Th; Warren, G A; Weis, M

    arXiv.org, 10/2000
    Paper

    The recoil proton polarization has been measured in the p (\vec e,e'\vec p) pi^0 reaction in parallel kinematics around W = 1232 MeV, Q^2 = 0.121 (GeV/c)^2 and epsilon = 0.718 using the polarized c.w. electron beam of the Mainz Microtron. Due to the spin precession in a magnetic spectrometer, all three proton polarization components P_x/P_e = (-11.4 \pm 1.3 \pm 1.4) %, P_y = (-43.1 \pm 1.3 \pm 2.2) %, and P_z/P_e = (56.2 \pm 1.5 \pm 2.6) % could be measured simultaneously. The Coulomb quadrupole to magnetic dipole ratio CMR = (-6.4\pm 0.7_{stat}\pm 0.8_{syst}) % was determined from P_x in the framework of the Mainz Unitary Isobar Model. The consistency among the reduced polarizations and the extraction of the ratio of longitudinal to transverse response is discussed.