{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:F546LRYJXUQMQ3FNHVR75EBDWY","short_pith_number":"pith:F546LRYJ","schema_version":"1.0","canonical_sha256":"2f79e5c709bd20c86cad3d63fe9023b633bebf7e1b73324bcba8fabbd6b792ef","source":{"kind":"arxiv","id":"1304.1976","version":1},"attestation_state":"computed","paper":{"title":"Neutron capture by 15N nucleus at astrophysical energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"N.V. Afanasyeva, S.B. Dubovichenko","submitted_at":"2013-04-07T10:04:39Z","abstract_excerpt":"Within the potential cluster model with the forbidden states and an orbital states classification according to the Young diagrams the possibility of description of experimental data for the total cross-sections of radiative n15N-capture at energies from 25 to 370 keV was considered. It was shown that only on basis of the E1-transitions from the different states of n15N-scattering to the ground state of 16N nucleus in n15N-channel it is well succeed to explain the value of the total cross-sections in the considered energy range and to prognosticate its behavior at energy E 1 eV. These cross-sec"},"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":"1304.1976","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-04-07T10:04:39Z","cross_cats_sorted":[],"title_canon_sha256":"893142ffbf363682bab1c1530b2153ea8c04bde1923e446c17476b3be3a91157","abstract_canon_sha256":"87b67652712aa55df6516c0c7aa43eb9b264e423e8192df8a15c65b0bb55214c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:50:41.982066Z","signature_b64":"N3M2umg0ZnrmNOBEs/o3Oj+YS1NgC/F7ard5r39wquUfEzWHu2EowqH5/X37Fx3Erh+9motypwe3ZrW8kKmnBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2f79e5c709bd20c86cad3d63fe9023b633bebf7e1b73324bcba8fabbd6b792ef","last_reissued_at":"2026-05-18T01:50:41.981423Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:50:41.981423Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Neutron capture by 15N nucleus at astrophysical energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"N.V. Afanasyeva, S.B. Dubovichenko","submitted_at":"2013-04-07T10:04:39Z","abstract_excerpt":"Within the potential cluster model with the forbidden states and an orbital states classification according to the Young diagrams the possibility of description of experimental data for the total cross-sections of radiative n15N-capture at energies from 25 to 370 keV was considered. It was shown that only on basis of the E1-transitions from the different states of n15N-scattering to the ground state of 16N nucleus in n15N-channel it is well succeed to explain the value of the total cross-sections in the considered energy range and to prognosticate its behavior at energy E 1 eV. These cross-sec"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1304.1976","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":"1304.1976","created_at":"2026-05-18T01:50:41.981526+00:00"},{"alias_kind":"arxiv_version","alias_value":"1304.1976v1","created_at":"2026-05-18T01:50:41.981526+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1304.1976","created_at":"2026-05-18T01:50:41.981526+00:00"},{"alias_kind":"pith_short_12","alias_value":"F546LRYJXUQM","created_at":"2026-05-18T12:27:43.054852+00:00"},{"alias_kind":"pith_short_16","alias_value":"F546LRYJXUQMQ3FN","created_at":"2026-05-18T12:27:43.054852+00:00"},{"alias_kind":"pith_short_8","alias_value":"F546LRYJ","created_at":"2026-05-18T12:27:43.054852+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/F546LRYJXUQMQ3FNHVR75EBDWY","json":"https://pith.science/pith/F546LRYJXUQMQ3FNHVR75EBDWY.json","graph_json":"https://pith.science/api/pith-number/F546LRYJXUQMQ3FNHVR75EBDWY/graph.json","events_json":"https://pith.science/api/pith-number/F546LRYJXUQMQ3FNHVR75EBDWY/events.json","paper":"https://pith.science/paper/F546LRYJ"},"agent_actions":{"view_html":"https://pith.science/pith/F546LRYJXUQMQ3FNHVR75EBDWY","download_json":"https://pith.science/pith/F546LRYJXUQMQ3FNHVR75EBDWY.json","view_paper":"https://pith.science/paper/F546LRYJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1304.1976&json=true","fetch_graph":"https://pith.science/api/pith-number/F546LRYJXUQMQ3FNHVR75EBDWY/graph.json","fetch_events":"https://pith.science/api/pith-number/F546LRYJXUQMQ3FNHVR75EBDWY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F546LRYJXUQMQ3FNHVR75EBDWY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F546LRYJXUQMQ3FNHVR75EBDWY/action/storage_attestation","attest_author":"https://pith.science/pith/F546LRYJXUQMQ3FNHVR75EBDWY/action/author_attestation","sign_citation":"https://pith.science/pith/F546LRYJXUQMQ3FNHVR75EBDWY/action/citation_signature","submit_replication":"https://pith.science/pith/F546LRYJXUQMQ3FNHVR75EBDWY/action/replication_record"}},"created_at":"2026-05-18T01:50:41.981526+00:00","updated_at":"2026-05-18T01:50:41.981526+00:00"}