{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:4EYU3SJENTV6TOABLRYV3EVQQF","short_pith_number":"pith:4EYU3SJE","schema_version":"1.0","canonical_sha256":"e1314dc9246cebe9b8015c715d92b08162962797dfe12e5c4ff2795eca3832fd","source":{"kind":"arxiv","id":"2010.07793","version":1},"attestation_state":"computed","paper":{"title":"A fully microscopic model of total level density in spherical nuclei","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"L. Tan Phuc, N. Dinh Dang, N. Ngoc Anh, N. Quang Hung, T. Dong Xuan, T. V. Nhan Hao","submitted_at":"2020-10-15T14:34:48Z","abstract_excerpt":"A fully microscopic model for the description of nuclear level density (NLD) in spherical nuclei is proposed. The model is derived by combining the partition function of the exact pairing solution plus the independent-particle model at finite temperature (EP+IPM) with that obtained by using the collective vibrational states calculated from the self-consistent Hartree-Fock mean field with MSk3 interaction plus the exact pairing and random-phases approximation (SC-HFEPRPA). Two important factors are taken into account in a fully microscopic way, namely the spin cut-off and vibrational enhancemen"},"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":"2010.07793","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2020-10-15T14:34:48Z","cross_cats_sorted":[],"title_canon_sha256":"ea0a687e2417b598a310528487099214a66b722c92d613c4ab1aec12ad34c5cf","abstract_canon_sha256":"0f495cddec5c5eadcb26c593c5c6238c09869031bd9fb878acbd3eae35e1ad45"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:56:12.913112Z","signature_b64":"XcEvOTmvwAskLTxrjyME6DzzunhQ+VzJ+HIhEBmNxYLavga8JdvBZfzK44WtIobbmjkFyjppms6r2xMv5aEYDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e1314dc9246cebe9b8015c715d92b08162962797dfe12e5c4ff2795eca3832fd","last_reissued_at":"2026-07-05T01:56:12.912774Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:56:12.912774Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A fully microscopic model of total level density in spherical nuclei","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"L. Tan Phuc, N. Dinh Dang, N. Ngoc Anh, N. Quang Hung, T. Dong Xuan, T. V. Nhan Hao","submitted_at":"2020-10-15T14:34:48Z","abstract_excerpt":"A fully microscopic model for the description of nuclear level density (NLD) in spherical nuclei is proposed. The model is derived by combining the partition function of the exact pairing solution plus the independent-particle model at finite temperature (EP+IPM) with that obtained by using the collective vibrational states calculated from the self-consistent Hartree-Fock mean field with MSk3 interaction plus the exact pairing and random-phases approximation (SC-HFEPRPA). Two important factors are taken into account in a fully microscopic way, namely the spin cut-off and vibrational enhancemen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2010.07793","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/2010.07793/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":"2010.07793","created_at":"2026-07-05T01:56:12.912831+00:00"},{"alias_kind":"arxiv_version","alias_value":"2010.07793v1","created_at":"2026-07-05T01:56:12.912831+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2010.07793","created_at":"2026-07-05T01:56:12.912831+00:00"},{"alias_kind":"pith_short_12","alias_value":"4EYU3SJENTV6","created_at":"2026-07-05T01:56:12.912831+00:00"},{"alias_kind":"pith_short_16","alias_value":"4EYU3SJENTV6TOAB","created_at":"2026-07-05T01:56:12.912831+00:00"},{"alias_kind":"pith_short_8","alias_value":"4EYU3SJE","created_at":"2026-07-05T01:56:12.912831+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/4EYU3SJENTV6TOABLRYV3EVQQF","json":"https://pith.science/pith/4EYU3SJENTV6TOABLRYV3EVQQF.json","graph_json":"https://pith.science/api/pith-number/4EYU3SJENTV6TOABLRYV3EVQQF/graph.json","events_json":"https://pith.science/api/pith-number/4EYU3SJENTV6TOABLRYV3EVQQF/events.json","paper":"https://pith.science/paper/4EYU3SJE"},"agent_actions":{"view_html":"https://pith.science/pith/4EYU3SJENTV6TOABLRYV3EVQQF","download_json":"https://pith.science/pith/4EYU3SJENTV6TOABLRYV3EVQQF.json","view_paper":"https://pith.science/paper/4EYU3SJE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2010.07793&json=true","fetch_graph":"https://pith.science/api/pith-number/4EYU3SJENTV6TOABLRYV3EVQQF/graph.json","fetch_events":"https://pith.science/api/pith-number/4EYU3SJENTV6TOABLRYV3EVQQF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4EYU3SJENTV6TOABLRYV3EVQQF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4EYU3SJENTV6TOABLRYV3EVQQF/action/storage_attestation","attest_author":"https://pith.science/pith/4EYU3SJENTV6TOABLRYV3EVQQF/action/author_attestation","sign_citation":"https://pith.science/pith/4EYU3SJENTV6TOABLRYV3EVQQF/action/citation_signature","submit_replication":"https://pith.science/pith/4EYU3SJENTV6TOABLRYV3EVQQF/action/replication_record"}},"created_at":"2026-07-05T01:56:12.912831+00:00","updated_at":"2026-07-05T01:56:12.912831+00:00"}