{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:N3YN4UXRURHLMNYSACBCB3EFRD","short_pith_number":"pith:N3YN4UXR","canonical_record":{"source":{"id":"1602.04027","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-02-12T12:11:24Z","cross_cats_sorted":[],"title_canon_sha256":"ce9040d9bf6f6d6242848cda435e30621b007656ebdc678a98fe8b51ac579b23","abstract_canon_sha256":"3b9b470f9d7ad5d389a7c3d47e9f4e416a11e38463f1e03bfb30108e81820572"},"schema_version":"1.0"},"canonical_sha256":"6ef0de52f1a44eb63712008220ec8588c1ec0eb858a68cbe6d4620e0f9174aef","source":{"kind":"arxiv","id":"1602.04027","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.04027","created_at":"2026-05-18T01:20:54Z"},{"alias_kind":"arxiv_version","alias_value":"1602.04027v1","created_at":"2026-05-18T01:20:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.04027","created_at":"2026-05-18T01:20:54Z"},{"alias_kind":"pith_short_12","alias_value":"N3YN4UXRURHL","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"N3YN4UXRURHLMNYS","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"N3YN4UXR","created_at":"2026-05-18T12:30:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:N3YN4UXRURHLMNYSACBCB3EFRD","target":"record","payload":{"canonical_record":{"source":{"id":"1602.04027","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-02-12T12:11:24Z","cross_cats_sorted":[],"title_canon_sha256":"ce9040d9bf6f6d6242848cda435e30621b007656ebdc678a98fe8b51ac579b23","abstract_canon_sha256":"3b9b470f9d7ad5d389a7c3d47e9f4e416a11e38463f1e03bfb30108e81820572"},"schema_version":"1.0"},"canonical_sha256":"6ef0de52f1a44eb63712008220ec8588c1ec0eb858a68cbe6d4620e0f9174aef","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:20:54.808269Z","signature_b64":"kDVTjyJaEVaeLjDld/I9oK8FNKrNcOz9715+zZ8hkMC4JRHwfHT9ul1I63EUlkFXrhXfBUiiJ2mv4vKLXTGxDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6ef0de52f1a44eb63712008220ec8588c1ec0eb858a68cbe6d4620e0f9174aef","last_reissued_at":"2026-05-18T01:20:54.807619Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:20:54.807619Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1602.04027","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:20:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ClSqPtLof0twuN9tdouiSlCN1xTSvL/Ec9zsfFEui26fPhoDIM7My7qxX6aArnz3MpmEDutzXw9YAADxPRBJCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T10:42:21.402332Z"},"content_sha256":"f0b9e8bd40cbd8cb7fd7465aa58adcc22cb12d31b63a65deb9163cdffc942a2f","schema_version":"1.0","event_id":"sha256:f0b9e8bd40cbd8cb7fd7465aa58adcc22cb12d31b63a65deb9163cdffc942a2f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:N3YN4UXRURHLMNYSACBCB3EFRD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Radiative rates for E1, E2, M1, and M2 transitions in S-like to F-like tungsten ions (W LIX to W LXVI)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"F P Keenan, K M Aggarwal","submitted_at":"2016-02-12T12:11:24Z","abstract_excerpt":"Calculations of energy levels, radiative rates and lifetimes are reported for eight ions of tungsten, i.e. S-like (W LIX) to F-like (W LXVI). A large number of levels has been considered for each ion and extensive configuration interaction has been included among a range of configurations. For the calculations, the general-purpose relativistic atomic structure package (GRASP) has been adopted, and radiative rates (as well as oscillator strengths and line strengths) are listed for all E1, E2, M1, and M2 transitions of the ions. Comparisons have been made with earlier available experimental and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.04027","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:20:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8zAjuK7YVZ9OVK8PcG0gwxVfB6F5AOR0XJ3ED72TwxBpxPwioyri65ILdea8maRq1YwlZqTlMtPNMBmkQ7i9Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T10:42:21.402681Z"},"content_sha256":"710c9598a35cb7079739f29d40ce5bfd5f446695d4691d76fe5a07503ae38c24","schema_version":"1.0","event_id":"sha256:710c9598a35cb7079739f29d40ce5bfd5f446695d4691d76fe5a07503ae38c24"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/N3YN4UXRURHLMNYSACBCB3EFRD/bundle.json","state_url":"https://pith.science/pith/N3YN4UXRURHLMNYSACBCB3EFRD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/N3YN4UXRURHLMNYSACBCB3EFRD/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-26T10:42:21Z","links":{"resolver":"https://pith.science/pith/N3YN4UXRURHLMNYSACBCB3EFRD","bundle":"https://pith.science/pith/N3YN4UXRURHLMNYSACBCB3EFRD/bundle.json","state":"https://pith.science/pith/N3YN4UXRURHLMNYSACBCB3EFRD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/N3YN4UXRURHLMNYSACBCB3EFRD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:N3YN4UXRURHLMNYSACBCB3EFRD","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":"3b9b470f9d7ad5d389a7c3d47e9f4e416a11e38463f1e03bfb30108e81820572","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-02-12T12:11:24Z","title_canon_sha256":"ce9040d9bf6f6d6242848cda435e30621b007656ebdc678a98fe8b51ac579b23"},"schema_version":"1.0","source":{"id":"1602.04027","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.04027","created_at":"2026-05-18T01:20:54Z"},{"alias_kind":"arxiv_version","alias_value":"1602.04027v1","created_at":"2026-05-18T01:20:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.04027","created_at":"2026-05-18T01:20:54Z"},{"alias_kind":"pith_short_12","alias_value":"N3YN4UXRURHL","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"N3YN4UXRURHLMNYS","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"N3YN4UXR","created_at":"2026-05-18T12:30:32Z"}],"graph_snapshots":[{"event_id":"sha256:710c9598a35cb7079739f29d40ce5bfd5f446695d4691d76fe5a07503ae38c24","target":"graph","created_at":"2026-05-18T01:20:54Z","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 eight ions of tungsten, i.e. S-like (W LIX) to F-like (W LXVI). A large number of levels has been considered for each ion and extensive configuration interaction has been included among a range of configurations. For the calculations, the general-purpose relativistic atomic structure package (GRASP) has been adopted, and radiative rates (as well as oscillator strengths and line strengths) are listed for all E1, E2, M1, and M2 transitions of the ions. Comparisons have been made with earlier available experimental and ","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":"2016-02-12T12:11:24Z","title":"Radiative rates for E1, E2, M1, and M2 transitions in S-like to F-like tungsten ions (W LIX to W LXVI)"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.04027","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:f0b9e8bd40cbd8cb7fd7465aa58adcc22cb12d31b63a65deb9163cdffc942a2f","target":"record","created_at":"2026-05-18T01:20:54Z","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":"3b9b470f9d7ad5d389a7c3d47e9f4e416a11e38463f1e03bfb30108e81820572","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-02-12T12:11:24Z","title_canon_sha256":"ce9040d9bf6f6d6242848cda435e30621b007656ebdc678a98fe8b51ac579b23"},"schema_version":"1.0","source":{"id":"1602.04027","kind":"arxiv","version":1}},"canonical_sha256":"6ef0de52f1a44eb63712008220ec8588c1ec0eb858a68cbe6d4620e0f9174aef","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6ef0de52f1a44eb63712008220ec8588c1ec0eb858a68cbe6d4620e0f9174aef","first_computed_at":"2026-05-18T01:20:54.807619Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:20:54.807619Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"kDVTjyJaEVaeLjDld/I9oK8FNKrNcOz9715+zZ8hkMC4JRHwfHT9ul1I63EUlkFXrhXfBUiiJ2mv4vKLXTGxDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:20:54.808269Z","signed_message":"canonical_sha256_bytes"},"source_id":"1602.04027","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f0b9e8bd40cbd8cb7fd7465aa58adcc22cb12d31b63a65deb9163cdffc942a2f","sha256:710c9598a35cb7079739f29d40ce5bfd5f446695d4691d76fe5a07503ae38c24"],"state_sha256":"5fbfaa15e6254df1353f94ba771eaf4b9c5f265d4d87aa61bc442069b9f28663"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"snaOpzkAb+Bm5UoQMF0WYrqCNKA3D2EHq/L5lPmddNTkkpAprXIZNOy0vfy9Z1E+R6K8Tg7DGF8WKkLgpRldDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-26T10:42:21.404556Z","bundle_sha256":"f46c403460b47e602a2d8c9cc8edaf623e59882bf22873b7da2aea18d422d2fa"}}