{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:JJDJR6AJKRKJQRNHU5R42LGGW3","short_pith_number":"pith:JJDJR6AJ","schema_version":"1.0","canonical_sha256":"4a4698f80954549845a7a763cd2cc6b6fcd932db310cc169c4863711c84d7d27","source":{"kind":"arxiv","id":"1604.08635","version":1},"attestation_state":"computed","paper":{"title":"Statistical Hauser-Feshbach theory with width fluctuation correction including direct reaction channels for neutron induced reaction at low energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"R. Capote, S. Hilaire, T. Kawano","submitted_at":"2016-04-28T22:16:35Z","abstract_excerpt":"A model to calculate particle-induced reaction cross sections with statistical Hauser-Feshbach theory including direct reactions is given. The energy average of scattering matrix from the coupled-channels optical model is diagonalized by the transformation proposed by Engelbrecht and Weidenm\\\"{u}ller. The ensemble average of $S$-matrix elements in the diagonalized channel space is approximated by a model of Moldauer [Phys.Rev.C {\\bf 12}, 744 (1975)] using newly parametrized channel degree-of-freedom $\\nu_a$ to better describe the Gaussian Orthogonal Ensemble (GOE) reference calculations. Molda"},"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":"1604.08635","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-04-28T22:16:35Z","cross_cats_sorted":[],"title_canon_sha256":"d0835c1840ab6c9a2d1c7d9ea67cd9281dcfab0a540f18949ff876ff1202afbe","abstract_canon_sha256":"edd8e798a289b664870403cd70f145b85219711fe8c95163de5d70bc950c9674"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:09.662996Z","signature_b64":"udyAoapNaZd67pIIznsQBhbebvOI8VaJOYFX7YjVYqVHPFGylbPpb4pYNBb0OIW1v13tHvzbDAPiHVCKgx5pCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4a4698f80954549845a7a763cd2cc6b6fcd932db310cc169c4863711c84d7d27","last_reissued_at":"2026-05-18T01:08:09.662607Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:09.662607Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Statistical Hauser-Feshbach theory with width fluctuation correction including direct reaction channels for neutron induced reaction at low energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"R. Capote, S. Hilaire, T. Kawano","submitted_at":"2016-04-28T22:16:35Z","abstract_excerpt":"A model to calculate particle-induced reaction cross sections with statistical Hauser-Feshbach theory including direct reactions is given. The energy average of scattering matrix from the coupled-channels optical model is diagonalized by the transformation proposed by Engelbrecht and Weidenm\\\"{u}ller. The ensemble average of $S$-matrix elements in the diagonalized channel space is approximated by a model of Moldauer [Phys.Rev.C {\\bf 12}, 744 (1975)] using newly parametrized channel degree-of-freedom $\\nu_a$ to better describe the Gaussian Orthogonal Ensemble (GOE) reference calculations. Molda"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.08635","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":""},"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":"1604.08635","created_at":"2026-05-18T01:08:09.662674+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.08635v1","created_at":"2026-05-18T01:08:09.662674+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.08635","created_at":"2026-05-18T01:08:09.662674+00:00"},{"alias_kind":"pith_short_12","alias_value":"JJDJR6AJKRKJ","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_16","alias_value":"JJDJR6AJKRKJQRNH","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_8","alias_value":"JJDJR6AJ","created_at":"2026-05-18T12:30:25.849896+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/JJDJR6AJKRKJQRNHU5R42LGGW3","json":"https://pith.science/pith/JJDJR6AJKRKJQRNHU5R42LGGW3.json","graph_json":"https://pith.science/api/pith-number/JJDJR6AJKRKJQRNHU5R42LGGW3/graph.json","events_json":"https://pith.science/api/pith-number/JJDJR6AJKRKJQRNHU5R42LGGW3/events.json","paper":"https://pith.science/paper/JJDJR6AJ"},"agent_actions":{"view_html":"https://pith.science/pith/JJDJR6AJKRKJQRNHU5R42LGGW3","download_json":"https://pith.science/pith/JJDJR6AJKRKJQRNHU5R42LGGW3.json","view_paper":"https://pith.science/paper/JJDJR6AJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.08635&json=true","fetch_graph":"https://pith.science/api/pith-number/JJDJR6AJKRKJQRNHU5R42LGGW3/graph.json","fetch_events":"https://pith.science/api/pith-number/JJDJR6AJKRKJQRNHU5R42LGGW3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JJDJR6AJKRKJQRNHU5R42LGGW3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JJDJR6AJKRKJQRNHU5R42LGGW3/action/storage_attestation","attest_author":"https://pith.science/pith/JJDJR6AJKRKJQRNHU5R42LGGW3/action/author_attestation","sign_citation":"https://pith.science/pith/JJDJR6AJKRKJQRNHU5R42LGGW3/action/citation_signature","submit_replication":"https://pith.science/pith/JJDJR6AJKRKJQRNHU5R42LGGW3/action/replication_record"}},"created_at":"2026-05-18T01:08:09.662674+00:00","updated_at":"2026-05-18T01:08:09.662674+00:00"}