{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:RZ4Y2EKE4UHZEUNUP7VV7P2HAY","short_pith_number":"pith:RZ4Y2EKE","schema_version":"1.0","canonical_sha256":"8e798d1144e50f9251b47feb5fbf470613105357a2a54f51207065eb0deff7d3","source":{"kind":"arxiv","id":"nucl-ex/0301016","version":3},"attestation_state":"computed","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."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"nucl-ex/0301016","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"nucl-ex","submitted_at":"2003-01-27T15:51:25Z","cross_cats_sorted":[],"title_canon_sha256":"61d799ad3662cc91f617ac223b69e20fc8d034fc9743c1d5e4a2e8402fd177c7","abstract_canon_sha256":"e9b19a4c2cbfdbd69694a6d29a1eca951fce387d93a6aa53afd867db7cd14050"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:13:46.131469Z","signature_b64":"OBeNZIo1iBN/tvdcMH+i4QVLGGHLYojlyGBKjxipKZjeLnUu7JF0MlmxWpPLBtWwIoRrXmtP2yuMRjEqDjQ7Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8e798d1144e50f9251b47feb5fbf470613105357a2a54f51207065eb0deff7d3","last_reissued_at":"2026-05-18T04:13:46.130980Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:13:46.130980Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"nucl-ex/0301016","created_at":"2026-05-18T04:13:46.131055+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-ex/0301016v3","created_at":"2026-05-18T04:13:46.131055+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-ex/0301016","created_at":"2026-05-18T04:13:46.131055+00:00"},{"alias_kind":"pith_short_12","alias_value":"RZ4Y2EKE4UHZ","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_16","alias_value":"RZ4Y2EKE4UHZEUNU","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_8","alias_value":"RZ4Y2EKE","created_at":"2026-05-18T12:25:52.051335+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RZ4Y2EKE4UHZEUNUP7VV7P2HAY","json":"https://pith.science/pith/RZ4Y2EKE4UHZEUNUP7VV7P2HAY.json","graph_json":"https://pith.science/api/pith-number/RZ4Y2EKE4UHZEUNUP7VV7P2HAY/graph.json","events_json":"https://pith.science/api/pith-number/RZ4Y2EKE4UHZEUNUP7VV7P2HAY/events.json","paper":"https://pith.science/paper/RZ4Y2EKE"},"agent_actions":{"view_html":"https://pith.science/pith/RZ4Y2EKE4UHZEUNUP7VV7P2HAY","download_json":"https://pith.science/pith/RZ4Y2EKE4UHZEUNUP7VV7P2HAY.json","view_paper":"https://pith.science/paper/RZ4Y2EKE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-ex/0301016&json=true","fetch_graph":"https://pith.science/api/pith-number/RZ4Y2EKE4UHZEUNUP7VV7P2HAY/graph.json","fetch_events":"https://pith.science/api/pith-number/RZ4Y2EKE4UHZEUNUP7VV7P2HAY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RZ4Y2EKE4UHZEUNUP7VV7P2HAY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RZ4Y2EKE4UHZEUNUP7VV7P2HAY/action/storage_attestation","attest_author":"https://pith.science/pith/RZ4Y2EKE4UHZEUNUP7VV7P2HAY/action/author_attestation","sign_citation":"https://pith.science/pith/RZ4Y2EKE4UHZEUNUP7VV7P2HAY/action/citation_signature","submit_replication":"https://pith.science/pith/RZ4Y2EKE4UHZEUNUP7VV7P2HAY/action/replication_record"}},"created_at":"2026-05-18T04:13:46.131055+00:00","updated_at":"2026-05-18T04:13:46.131055+00:00"}