{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:AA3H4MW4IKM4REO7QVSKDJOJL2","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"eeb30e114dba3f94fedc8c6816eab22e5c18191ff779ff02231e03e29ae86236","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2013-07-01T15:17:23Z","title_canon_sha256":"1b5c3e7a8fbfaf6703c8f6927e663e1f1c55b146247be4e6d9fe9e6e5c36a0cc"},"schema_version":"1.0","source":{"id":"1307.0404","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.0404","created_at":"2026-05-18T01:49:01Z"},{"alias_kind":"arxiv_version","alias_value":"1307.0404v2","created_at":"2026-05-18T01:49:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.0404","created_at":"2026-05-18T01:49:01Z"},{"alias_kind":"pith_short_12","alias_value":"AA3H4MW4IKM4","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"AA3H4MW4IKM4REO7","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"AA3H4MW4","created_at":"2026-05-18T12:27:38Z"}],"graph_snapshots":[{"event_id":"sha256:e7304c24b0f991d671966e284eb2acfacd13e92609ee6454266994518dcb483a","target":"graph","created_at":"2026-05-18T01:49:01Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"The hyperfine interaction constants of the 2p4(3P)3p 2Do_{3/2,5/2}, 4Do_{1/2-7/2} and 4Po_{1/2-5/2} levels in neutral fluorine are investigated theoretically. Large-scale calculations are carried out using the multiconfiguration Hartree-Fock (MCHF) and Dirac-Hartree-Fock (MCDHF) methods. In the framework of the MCHF approach, the relativistic effects are taken into account in the Breit-Pauli approximation using non relativistic orbitals. In the fully relativistic approach, the orbitals are optimized using the Dirac-Coulomb Hamiltonian with correlation models inspired by the non relativistic ca","authors_text":"Jiguang Li, Messaoud Nemouchi, Michel Godefroid, Thomas Carette","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2013-07-01T15:17:23Z","title":"Relativistic effects on the hyperfine structures of 2p4(3P)3p 2Do, 4Do and 4Po in 19F I"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.0404","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:fd335de049ebaf40da95724ca11a39735429050a6ef358b987f538c3a53abcfd","target":"record","created_at":"2026-05-18T01:49:01Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"eeb30e114dba3f94fedc8c6816eab22e5c18191ff779ff02231e03e29ae86236","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2013-07-01T15:17:23Z","title_canon_sha256":"1b5c3e7a8fbfaf6703c8f6927e663e1f1c55b146247be4e6d9fe9e6e5c36a0cc"},"schema_version":"1.0","source":{"id":"1307.0404","kind":"arxiv","version":2}},"canonical_sha256":"00367e32dc4299c891df8564a1a5c95eaa7cf3075f28f8278346da32164af133","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"00367e32dc4299c891df8564a1a5c95eaa7cf3075f28f8278346da32164af133","first_computed_at":"2026-05-18T01:49:01.126892Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:49:01.126892Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bB054bWtCRYmiG5jCySTdsV1JpJ3xGbZ0jo6/uImO9vwE0S5Ue3YWtrSGQuqi0RD30UTa6sn9f33DV5gQt5HBA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:49:01.127337Z","signed_message":"canonical_sha256_bytes"},"source_id":"1307.0404","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fd335de049ebaf40da95724ca11a39735429050a6ef358b987f538c3a53abcfd","sha256:e7304c24b0f991d671966e284eb2acfacd13e92609ee6454266994518dcb483a"],"state_sha256":"166091f108ab962ecab42fcba4cbe58be856467c83d035dd42a552a5ac49e0cb"}