Measurement of the recoil polarization in the p (\vec e, e' \vec p) pi^0 reaction at the Δ(1232) resonance
| dc.creator | Pospischil, Th. | |
| dc.creator | Bartsch, P. | |
| dc.creator | Baumann, D. | |
| dc.creator | Bermuth, J. | |
| dc.creator | Boehm, R. | |
| dc.creator | Bohinc, K. | |
| dc.creator | Derber, S. | |
| dc.creator | Ding, M. | |
| dc.creator | Distler, M. | |
| dc.creator | Drechsel, D. | |
| dc.creator | Elsner, D. | |
| dc.creator | Ewald, I. | |
| dc.creator | Friedrich, J. | |
| dc.creator | Friedrich, J. M. | |
| dc.creator | Geiges, R. | |
| dc.creator | Hedicke, S. | |
| dc.creator | Jennewein, P. | |
| dc.creator | Kahrau, M. | |
| dc.creator | Kamalov, S. S. | |
| dc.creator | Klein, F. | |
| dc.creator | Krygier, K. W. | |
| dc.creator | Lac, J. | |
| dc.creator | Liesenfeld, A. | |
| dc.creator | McIntyre, J. | |
| dc.creator | Merkel, H. | |
| dc.creator | Merle, P. | |
| dc.creator | Mueller, U. | |
| dc.creator | Neuhausen, R. | |
| dc.creator | Potokar, M. | |
| dc.creator | Ransome, R. D. | |
| dc.creator | Rohe, D. | |
| dc.creator | Rosner, G. | |
| dc.creator | Schmieden, H. | |
| dc.creator | Seimetz, M. | |
| dc.creator | Sirca, S. | |
| dc.creator | Sick, I. | |
| dc.creator | Suele, A. | |
| dc.creator | Tiator, L. | |
| dc.creator | Wagner, A. | |
| dc.creator | Walcher, Th | |
| dc.creator | Warren, G. A. | |
| dc.creator | Weis, M. | |
| dc.date | 2000-10-31 | |
| dc.date.accessioned | 2026-07-07T11:32:28Z | |
| dc.date.available | 2026-07-07T11:32:28Z | |
| dc.description | 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. | |
| dc.description | 5 pages LaTeX, 1 table, 2 eps figures | |
| dc.identifier | https://arxiv.org/abs/nucl-ex/0010020 | |
| dc.identifier | http://arxiv.org/abs/nucl-ex/0010020 | |
| dc.identifier | Phys.Rev.Lett.86:2959-2962,2001 | |
| dc.identifier | doi:10.1103/PhysRevLett.86.2959 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/197605 | |
| dc.subject | Nuclear Experiment | |
| dc.title | Measurement of the recoil polarization in the p (\vec e, e' \vec p) pi^0 reaction at the Δ(1232) resonance | |
| dc.type | text |