{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:ZVZ2OIUYETGBNX4H75T55LZDHR","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":"8f5a0fcfede5f29be259364aa492e4ebe1d524555f35db2fa57b9c1d1af2f9bd","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-12-01T15:16:44Z","title_canon_sha256":"6eb2a0b1dbd40dad0c96eb8ee99f0607edb3c15d247b9fbd57bdc1af50b43771"},"schema_version":"1.0","source":{"id":"1512.00291","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.00291","created_at":"2026-05-18T01:25:32Z"},{"alias_kind":"arxiv_version","alias_value":"1512.00291v1","created_at":"2026-05-18T01:25:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.00291","created_at":"2026-05-18T01:25:32Z"},{"alias_kind":"pith_short_12","alias_value":"ZVZ2OIUYETGB","created_at":"2026-05-18T12:29:52Z"},{"alias_kind":"pith_short_16","alias_value":"ZVZ2OIUYETGBNX4H","created_at":"2026-05-18T12:29:52Z"},{"alias_kind":"pith_short_8","alias_value":"ZVZ2OIUY","created_at":"2026-05-18T12:29:52Z"}],"graph_snapshots":[{"event_id":"sha256:8e9b395c7fe711408944c6f7f3304f886737e895d7a727271ddf1d0067567045","target":"graph","created_at":"2026-05-18T01:25:32Z","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":"Calculations of energy levels, radiative rates and lifetimes are reported for 17 F-like ions with 37 $\\le$ Z $\\le$ 53. For brevity, results are only presented among the lowest 113 levels of the 2s$^2$2p$^5$, 2s2p$^6$, 2s$^2$2p$^4$3$\\ell$, 2s2p$^5$3$\\ell$, and 2p$^6$3$\\ell$ configurations, although the calculations have been performed for up to 501 levels in each ion. The general-purpose relativistic atomic structure package (GRASP) has been adopted for the calculations, and radiative rates (along with oscillator strengths and line strengths) are listed for all E1, E2, M1, and M2 transitions of","authors_text":"F P Keenan, K M Aggarwal","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-12-01T15:16:44Z","title":"Radiative rates for E1, E2, M1, and M2 transitions in F-like ions with 37 $\\le$ Z $\\le$ 53"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.00291","kind":"arxiv","version":1},"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":"sha256:0ff3eef40c9d2a3ed4a3c89a97b62d313930d3efe1c2299661c58c2dca704d98","target":"record","created_at":"2026-05-18T01:25:32Z","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":"8f5a0fcfede5f29be259364aa492e4ebe1d524555f35db2fa57b9c1d1af2f9bd","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-12-01T15:16:44Z","title_canon_sha256":"6eb2a0b1dbd40dad0c96eb8ee99f0607edb3c15d247b9fbd57bdc1af50b43771"},"schema_version":"1.0","source":{"id":"1512.00291","kind":"arxiv","version":1}},"canonical_sha256":"cd73a7229824cc16df87ff67deaf233c5b62bbe417e52e08d87ca93ff8c2ed36","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cd73a7229824cc16df87ff67deaf233c5b62bbe417e52e08d87ca93ff8c2ed36","first_computed_at":"2026-05-18T01:25:32.320797Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:25:32.320797Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mOebjkuhA6Z5A+GXNtjb5QFsZiHmvZfHiqrIye3xSMcx32bd7aPgvCup9mE/nrW3iGgggn7R5VrCZLX2k75KDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:25:32.321427Z","signed_message":"canonical_sha256_bytes"},"source_id":"1512.00291","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0ff3eef40c9d2a3ed4a3c89a97b62d313930d3efe1c2299661c58c2dca704d98","sha256:8e9b395c7fe711408944c6f7f3304f886737e895d7a727271ddf1d0067567045"],"state_sha256":"17c1e6c3f39fd0490664c083b95875682b84a763d955fd753232a20dcecd633b"}