{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:RMKTF25S7O3PHH4YRGKZWVK3FJ","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":"d21029608d52f539aa0c38abd23c92ffcd6133ef0df4faeee3065515858e6c30","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-01-07T17:47:27Z","title_canon_sha256":"27ccc8abadb7a266c023054213b3500ed58ff8391d1fb8e3e728963899cd9eec"},"schema_version":"1.0","source":{"id":"1901.02008","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1901.02008","created_at":"2026-05-17T23:56:16Z"},{"alias_kind":"arxiv_version","alias_value":"1901.02008v1","created_at":"2026-05-17T23:56:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.02008","created_at":"2026-05-17T23:56:16Z"},{"alias_kind":"pith_short_12","alias_value":"RMKTF25S7O3P","created_at":"2026-05-18T12:33:27Z"},{"alias_kind":"pith_short_16","alias_value":"RMKTF25S7O3PHH4Y","created_at":"2026-05-18T12:33:27Z"},{"alias_kind":"pith_short_8","alias_value":"RMKTF25S","created_at":"2026-05-18T12:33:27Z"}],"graph_snapshots":[{"event_id":"sha256:4d871da87b56bf27868f2cc58f91f4f6062a31c302fb09b951de533f3c9e7cf7","target":"graph","created_at":"2026-05-17T23:56:16Z","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":"In this paper, energy levels, radiative rates and lifetimes are reported for 11 F-like ions with 12 $\\le$ Z $\\le$ 23. Up to 198 levels (depending on the ion) have been considered which include 113 of the 2s$^2$2p$^5$, 2s2p$^6$, 2s$^2$2p$^4$3$\\ell$, 2s2p$^5$3$\\ell$, and 2p$^6$3$\\ell$ configurations. The general-purpose relativistic atomic structure package ({\\sc grasp}) and the flexible atomic code ({\\sc fac}) have been adopted for calculating the energy levels, but the {\\sc grasp} alone for the remaining parameters. Radiative rates (along with oscillator strengths and line strengths) are liste","authors_text":"K M Aggarwal","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-01-07T17:47:27Z","title":"Radiative rates for E1, E2, M1, and M2 transitions in F-like ions with 12 <= Z <= 23"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.02008","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":"sha256:7b7d9832d226952e9bc248f9983fc6cd6cd30ed427a9d2b18f4ba67151710848","target":"record","created_at":"2026-05-17T23:56:16Z","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":"d21029608d52f539aa0c38abd23c92ffcd6133ef0df4faeee3065515858e6c30","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-01-07T17:47:27Z","title_canon_sha256":"27ccc8abadb7a266c023054213b3500ed58ff8391d1fb8e3e728963899cd9eec"},"schema_version":"1.0","source":{"id":"1901.02008","kind":"arxiv","version":1}},"canonical_sha256":"8b1532ebb2fbb6f39f9889959b555b2a6ac5aa047628b1b95f31b1674f0a071f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8b1532ebb2fbb6f39f9889959b555b2a6ac5aa047628b1b95f31b1674f0a071f","first_computed_at":"2026-05-17T23:56:16.198274Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:56:16.198274Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yFIR7II4EJzSSGonjoZv3c7W+mbx6VQ+SIf2DC2Ko4OjYgyzj8ouDKHbCrpsgYEn/DJnndBh0dbSqwbnMEWzDA==","signature_status":"signed_v1","signed_at":"2026-05-17T23:56:16.198892Z","signed_message":"canonical_sha256_bytes"},"source_id":"1901.02008","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7b7d9832d226952e9bc248f9983fc6cd6cd30ed427a9d2b18f4ba67151710848","sha256:4d871da87b56bf27868f2cc58f91f4f6062a31c302fb09b951de533f3c9e7cf7"],"state_sha256":"31300dc5882d82c970d7d289e345d6618724ac8d26f827b640ea1dacbc68bd3b"}