{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:VIKZHY2TEHBZHXKAEW5LPGZAUI","short_pith_number":"pith:VIKZHY2T","schema_version":"1.0","canonical_sha256":"aa1593e35321c393dd4025bab79b20a21374b5133251ced59fe8077d892318f9","source":{"kind":"arxiv","id":"1310.0749","version":1},"attestation_state":"computed","paper":{"title":"Microscopic Calculation of Fusion: Light to Heavy Systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A.S. Umar, J.A. Maruhn, R. Keser, V.E. Oberacker","submitted_at":"2013-10-02T15:52:49Z","abstract_excerpt":"The density-constrained time-dependent Hartree-Fock (DC-TDHF) theory is a fully microscopic approach for calculating heavy-ion interaction potentials and fusion cross sections below and above the fusion barrier. We discuss recent applications of DC-TDHF method to fusion of light and heavy neutron-rich systems."},"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":"1310.0749","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-10-02T15:52:49Z","cross_cats_sorted":[],"title_canon_sha256":"820dbd76d473455c8e057bf60d7450a44f2d484b0cd70907d940d3d8f142237d","abstract_canon_sha256":"89aaa5f209362504aa5cd8e7526a6466325e3909f250754980ff4ebd5cd2fc78"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:02.206999Z","signature_b64":"yPqLcbwqThaJVFeCJoWPIn8BDqgY8kfG+wK96ZFEIWd/I7xtyWswtVOLUVz9FfWN3q9K+Qcyz2v71zzySyFQAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aa1593e35321c393dd4025bab79b20a21374b5133251ced59fe8077d892318f9","last_reissued_at":"2026-05-18T00:37:02.206266Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:02.206266Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Microscopic Calculation of Fusion: Light to Heavy Systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A.S. Umar, J.A. Maruhn, R. Keser, V.E. Oberacker","submitted_at":"2013-10-02T15:52:49Z","abstract_excerpt":"The density-constrained time-dependent Hartree-Fock (DC-TDHF) theory is a fully microscopic approach for calculating heavy-ion interaction potentials and fusion cross sections below and above the fusion barrier. We discuss recent applications of DC-TDHF method to fusion of light and heavy neutron-rich systems."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.0749","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":"1310.0749","created_at":"2026-05-18T00:37:02.206394+00:00"},{"alias_kind":"arxiv_version","alias_value":"1310.0749v1","created_at":"2026-05-18T00:37:02.206394+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.0749","created_at":"2026-05-18T00:37:02.206394+00:00"},{"alias_kind":"pith_short_12","alias_value":"VIKZHY2TEHBZ","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_16","alias_value":"VIKZHY2TEHBZHXKA","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_8","alias_value":"VIKZHY2T","created_at":"2026-05-18T12:28:04.890932+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/VIKZHY2TEHBZHXKAEW5LPGZAUI","json":"https://pith.science/pith/VIKZHY2TEHBZHXKAEW5LPGZAUI.json","graph_json":"https://pith.science/api/pith-number/VIKZHY2TEHBZHXKAEW5LPGZAUI/graph.json","events_json":"https://pith.science/api/pith-number/VIKZHY2TEHBZHXKAEW5LPGZAUI/events.json","paper":"https://pith.science/paper/VIKZHY2T"},"agent_actions":{"view_html":"https://pith.science/pith/VIKZHY2TEHBZHXKAEW5LPGZAUI","download_json":"https://pith.science/pith/VIKZHY2TEHBZHXKAEW5LPGZAUI.json","view_paper":"https://pith.science/paper/VIKZHY2T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1310.0749&json=true","fetch_graph":"https://pith.science/api/pith-number/VIKZHY2TEHBZHXKAEW5LPGZAUI/graph.json","fetch_events":"https://pith.science/api/pith-number/VIKZHY2TEHBZHXKAEW5LPGZAUI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VIKZHY2TEHBZHXKAEW5LPGZAUI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VIKZHY2TEHBZHXKAEW5LPGZAUI/action/storage_attestation","attest_author":"https://pith.science/pith/VIKZHY2TEHBZHXKAEW5LPGZAUI/action/author_attestation","sign_citation":"https://pith.science/pith/VIKZHY2TEHBZHXKAEW5LPGZAUI/action/citation_signature","submit_replication":"https://pith.science/pith/VIKZHY2TEHBZHXKAEW5LPGZAUI/action/replication_record"}},"created_at":"2026-05-18T00:37:02.206394+00:00","updated_at":"2026-05-18T00:37:02.206394+00:00"}