{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:CSIVK3ENOUMWKAFXEQLPTDVUA5","short_pith_number":"pith:CSIVK3EN","schema_version":"1.0","canonical_sha256":"1491556c8d75196500b72416f98eb4077ca04284e6d57b12bf924a7e13f5cff4","source":{"kind":"arxiv","id":"0801.3210","version":1},"attestation_state":"computed","paper":{"title":"Poincar\\'e Invariant Three-Body Scattering at Intermediate Energies","license":"","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Ch. Elster, H. Witala, T. Lin, W. Gloeckle, W.N. Polyzou","submitted_at":"2008-01-21T15:34:15Z","abstract_excerpt":"The relativistic Faddeev equation for three-nucleon scattering is formulated in momentum space and directly solved in terms of momentum vectors without employing a partial wave decomposition. The equation is solved through Pad\\'e summation, and the numerical feasibility and stability of the solution is demonstrated. Relativistic invariance is achieved by constructing a dynamical unitary representation of the Poincar\\'e group on the three-nucleon Hilbert space. Based on a Malfliet-Tjon type interaction, observables for elastic and break-up scattering are calculated for projectile energies in th"},"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":"0801.3210","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2008-01-21T15:34:15Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"eba2201a4b10d19548197592606113b014790ea0b44a4e6a8330e5b01b82b5f1","abstract_canon_sha256":"72319238bd6d82c660d49766c5c6bebe14d11d022026d15635d61087c5796ff8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:30:55.030662Z","signature_b64":"fiir67uIAxzhvsXSj0WfW9bZ42mxdjDPIoPNylwEoll9Nq/Vxyzk+cE0daasZzKb1ySMfHyJ3ppouEmuXJgTCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1491556c8d75196500b72416f98eb4077ca04284e6d57b12bf924a7e13f5cff4","last_reissued_at":"2026-07-04T15:30:55.030225Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:30:55.030225Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Poincar\\'e Invariant Three-Body Scattering at Intermediate Energies","license":"","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Ch. Elster, H. Witala, T. Lin, W. Gloeckle, W.N. Polyzou","submitted_at":"2008-01-21T15:34:15Z","abstract_excerpt":"The relativistic Faddeev equation for three-nucleon scattering is formulated in momentum space and directly solved in terms of momentum vectors without employing a partial wave decomposition. The equation is solved through Pad\\'e summation, and the numerical feasibility and stability of the solution is demonstrated. Relativistic invariance is achieved by constructing a dynamical unitary representation of the Poincar\\'e group on the three-nucleon Hilbert space. Based on a Malfliet-Tjon type interaction, observables for elastic and break-up scattering are calculated for projectile energies in th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0801.3210","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0801.3210/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"0801.3210","created_at":"2026-07-04T15:30:55.030282+00:00"},{"alias_kind":"arxiv_version","alias_value":"0801.3210v1","created_at":"2026-07-04T15:30:55.030282+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0801.3210","created_at":"2026-07-04T15:30:55.030282+00:00"},{"alias_kind":"pith_short_12","alias_value":"CSIVK3ENOUMW","created_at":"2026-07-04T15:30:55.030282+00:00"},{"alias_kind":"pith_short_16","alias_value":"CSIVK3ENOUMWKAFX","created_at":"2026-07-04T15:30:55.030282+00:00"},{"alias_kind":"pith_short_8","alias_value":"CSIVK3EN","created_at":"2026-07-04T15:30:55.030282+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/CSIVK3ENOUMWKAFXEQLPTDVUA5","json":"https://pith.science/pith/CSIVK3ENOUMWKAFXEQLPTDVUA5.json","graph_json":"https://pith.science/api/pith-number/CSIVK3ENOUMWKAFXEQLPTDVUA5/graph.json","events_json":"https://pith.science/api/pith-number/CSIVK3ENOUMWKAFXEQLPTDVUA5/events.json","paper":"https://pith.science/paper/CSIVK3EN"},"agent_actions":{"view_html":"https://pith.science/pith/CSIVK3ENOUMWKAFXEQLPTDVUA5","download_json":"https://pith.science/pith/CSIVK3ENOUMWKAFXEQLPTDVUA5.json","view_paper":"https://pith.science/paper/CSIVK3EN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0801.3210&json=true","fetch_graph":"https://pith.science/api/pith-number/CSIVK3ENOUMWKAFXEQLPTDVUA5/graph.json","fetch_events":"https://pith.science/api/pith-number/CSIVK3ENOUMWKAFXEQLPTDVUA5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CSIVK3ENOUMWKAFXEQLPTDVUA5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CSIVK3ENOUMWKAFXEQLPTDVUA5/action/storage_attestation","attest_author":"https://pith.science/pith/CSIVK3ENOUMWKAFXEQLPTDVUA5/action/author_attestation","sign_citation":"https://pith.science/pith/CSIVK3ENOUMWKAFXEQLPTDVUA5/action/citation_signature","submit_replication":"https://pith.science/pith/CSIVK3ENOUMWKAFXEQLPTDVUA5/action/replication_record"}},"created_at":"2026-07-04T15:30:55.030282+00:00","updated_at":"2026-07-04T15:30:55.030282+00:00"}