{"paper":{"title":"Final State Interaction Effects in pol 3He(pol e,e'p)","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. Klein, A. Nogga, C. Carasco, Ch. Normand, D. Baumann, D. Bosnar, D. Rohe, E. Otten, G. Testa, G. Warren, H. Kamada, H. Merkel, H. Schmieden, H. Witala, H. Woehrle, I. Sick, J. Bermuth, J. Friedrich, J. Golak, J. Jourdan, J. M. Friedrich, J. Schmiedeskamp, K. W. Krygier, M. Ding, M. Hauger, M. Kohl, M. O. Distler, M. Potokar, M. Seimetz, M. Weis, M. Zeier, P. Bartsch, P. Jennewein, P. Merle, R. Boehm, R. Neuhausen, R. Skibinski, S. Sirca, Th. Pospischil, Th. Walcher, U. Mueller, W. Gloeckle, W. Heil","submitted_at":"2003-01-27T15:51:25Z","abstract_excerpt":"Asymmetries in quasi-elastic pol 3He(pol e,e'p) have been measured at a momentum transfer of 0.67 (GeV/c)^2 and are compared to a calculation which takes into account relativistic kinematics in the final state and a relativistic one-body current operator. With an exact solution of the Faddeev equation for the 3He-ground state and an approximate treatment of final state interactions in the continuum good agreement is found with the experimental data."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-ex/0301016","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}