{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:KI6NHQROAQYATYU4LYYWUNGLMA","short_pith_number":"pith:KI6NHQRO","schema_version":"1.0","canonical_sha256":"523cd3c22e043009e29c5e316a34cb600ed05169058171fbda2f531c053a5e0b","source":{"kind":"arxiv","id":"nucl-ex/0511054","version":2},"attestation_state":"computed","paper":{"title":"Microcanonical entropies and radiative strength functions of $^{50,51}$V","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. C. Larsen, A. Schiller, A. Voinov, F. Ingebretsen, J. Rekstad, M. Guttormsen, N. U. H. Syed, R. Chankova, S. Messelt, S. Siem, S. W. {\\O}deg{\\aa}rd, T. L\\\"onnroth","submitted_at":"2005-11-30T09:25:28Z","abstract_excerpt":"The level densities and radiative strength functions (RSFs) of $^{50,51}$V have been extracted using the ($^3$He,$\\alpha \\gamma$) and ($^3$He,$^3$He$^{\\prime} \\gamma$) reactions, respectively. From the level densities, microcanonical entropies are deduced. The high $\\gamma$-energy part of the RSF is described by the giant electric dipole resonance. A significant enhancement over the predicted strength in the region of $E_{\\gamma} \\lesssim 3$ MeV is seen, which at present has no theoretical explanation."},"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/0511054","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-ex","submitted_at":"2005-11-30T09:25:28Z","cross_cats_sorted":[],"title_canon_sha256":"92d0a857cd799340bc80fa6efcd511c313054c133fe136bd6e375b3f8444f9ba","abstract_canon_sha256":"84242b06de86fe122f92eaa6d84127014386d23ff77bfeb9a991510f299ac66b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:48.996534Z","signature_b64":"EGJ3hKQKlOMAwzJpx3xXJau+VadxfGbce4mKqNuH+Muk8nS0bUtz4jPHXuL1UnoPEXH0TS7iAP13Tv19ugOhDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"523cd3c22e043009e29c5e316a34cb600ed05169058171fbda2f531c053a5e0b","last_reissued_at":"2026-05-18T01:08:48.996044Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:48.996044Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Microcanonical entropies and radiative strength functions of $^{50,51}$V","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. C. Larsen, A. Schiller, A. Voinov, F. Ingebretsen, J. Rekstad, M. Guttormsen, N. U. H. Syed, R. Chankova, S. Messelt, S. Siem, S. W. {\\O}deg{\\aa}rd, T. L\\\"onnroth","submitted_at":"2005-11-30T09:25:28Z","abstract_excerpt":"The level densities and radiative strength functions (RSFs) of $^{50,51}$V have been extracted using the ($^3$He,$\\alpha \\gamma$) and ($^3$He,$^3$He$^{\\prime} \\gamma$) reactions, respectively. From the level densities, microcanonical entropies are deduced. The high $\\gamma$-energy part of the RSF is described by the giant electric dipole resonance. A significant enhancement over the predicted strength in the region of $E_{\\gamma} \\lesssim 3$ MeV is seen, which at present has no theoretical explanation."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-ex/0511054","kind":"arxiv","version":2},"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/0511054","created_at":"2026-05-18T01:08:48.996123+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-ex/0511054v2","created_at":"2026-05-18T01:08:48.996123+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-ex/0511054","created_at":"2026-05-18T01:08:48.996123+00:00"},{"alias_kind":"pith_short_12","alias_value":"KI6NHQROAQYA","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_16","alias_value":"KI6NHQROAQYATYU4","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_8","alias_value":"KI6NHQRO","created_at":"2026-05-18T12:25:53.335082+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/KI6NHQROAQYATYU4LYYWUNGLMA","json":"https://pith.science/pith/KI6NHQROAQYATYU4LYYWUNGLMA.json","graph_json":"https://pith.science/api/pith-number/KI6NHQROAQYATYU4LYYWUNGLMA/graph.json","events_json":"https://pith.science/api/pith-number/KI6NHQROAQYATYU4LYYWUNGLMA/events.json","paper":"https://pith.science/paper/KI6NHQRO"},"agent_actions":{"view_html":"https://pith.science/pith/KI6NHQROAQYATYU4LYYWUNGLMA","download_json":"https://pith.science/pith/KI6NHQROAQYATYU4LYYWUNGLMA.json","view_paper":"https://pith.science/paper/KI6NHQRO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-ex/0511054&json=true","fetch_graph":"https://pith.science/api/pith-number/KI6NHQROAQYATYU4LYYWUNGLMA/graph.json","fetch_events":"https://pith.science/api/pith-number/KI6NHQROAQYATYU4LYYWUNGLMA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KI6NHQROAQYATYU4LYYWUNGLMA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KI6NHQROAQYATYU4LYYWUNGLMA/action/storage_attestation","attest_author":"https://pith.science/pith/KI6NHQROAQYATYU4LYYWUNGLMA/action/author_attestation","sign_citation":"https://pith.science/pith/KI6NHQROAQYATYU4LYYWUNGLMA/action/citation_signature","submit_replication":"https://pith.science/pith/KI6NHQROAQYATYU4LYYWUNGLMA/action/replication_record"}},"created_at":"2026-05-18T01:08:48.996123+00:00","updated_at":"2026-05-18T01:08:48.996123+00:00"}