{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:ISSNTP3WHNBTMLMJJ7MDZINALI","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":"d1eec329b9983ef37fc540b9431037c0e8be15c53e994446d1cd3b177a0f37a5","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-02-03T07:03:57Z","title_canon_sha256":"85cbe6a2bcb452855e28f30e42bc95d8088b42f184120ebbc994c1aa548e4d74"},"schema_version":"1.0","source":{"id":"2502.01112","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.01112","created_at":"2026-07-05T10:12:03Z"},{"alias_kind":"arxiv_version","alias_value":"2502.01112v2","created_at":"2026-07-05T10:12:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.01112","created_at":"2026-07-05T10:12:03Z"},{"alias_kind":"pith_short_12","alias_value":"ISSNTP3WHNBT","created_at":"2026-07-05T10:12:03Z"},{"alias_kind":"pith_short_16","alias_value":"ISSNTP3WHNBTMLMJ","created_at":"2026-07-05T10:12:03Z"},{"alias_kind":"pith_short_8","alias_value":"ISSNTP3W","created_at":"2026-07-05T10:12:03Z"}],"graph_snapshots":[{"event_id":"sha256:5c5d0db58b58f3312b1fa405c777f40f76156af3465c66b2abb4f774ccb96e12","target":"graph","created_at":"2026-07-05T10:12:03Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2502.01112/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The transition energies and properties of the Ir$^{17+}$ ion are calculated using the Kramers-restricted configuration-interaction (KRCI) and Fock-space coupled-cluster (FSCC) methods within the Dirac-Coulomb-Gaunt Hamiltonian framework. These calculations show several forbidden optical transitions between the $4f^{13}5s$ ground state and the $4f^{14}$ and $4f^{12}5s^2$ excited states, underscoring their potential as candidates for optical clock applications. Additionally, key properties of the ground and low-lying excited states are reported, including Lande $g_J$ factors, lifetimes, electric","authors_text":"B. B. Suo, H. X. Liu, Y. F. Ge, Y. Liu, Y. M. Yu","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-02-03T07:03:57Z","title":"Relativistic configuration-interaction and coupled-cluster calculations of Ir$^{17+}$ transition energies and properties for optical clock applications"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.01112","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:b7e46bd22f252e9b2bc06d10e803e516f321f701663b7c4d0af90141859a1f1f","target":"record","created_at":"2026-07-05T10:12:03Z","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":"d1eec329b9983ef37fc540b9431037c0e8be15c53e994446d1cd3b177a0f37a5","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-02-03T07:03:57Z","title_canon_sha256":"85cbe6a2bcb452855e28f30e42bc95d8088b42f184120ebbc994c1aa548e4d74"},"schema_version":"1.0","source":{"id":"2502.01112","kind":"arxiv","version":2}},"canonical_sha256":"44a4d9bf763b43362d894fd83ca1a05a2a828652f79aff307a7e2fa784c4096f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"44a4d9bf763b43362d894fd83ca1a05a2a828652f79aff307a7e2fa784c4096f","first_computed_at":"2026-07-05T10:12:03.662362Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:12:03.662362Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6gvD+DEYwi/eNhDzpuRvVP1eSwdiPPcs8JomAr8GPpLH4kbDZOnodXqyxUR1HiRvXgmILoPGmHAWjknm3nbjCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:12:03.663026Z","signed_message":"canonical_sha256_bytes"},"source_id":"2502.01112","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b7e46bd22f252e9b2bc06d10e803e516f321f701663b7c4d0af90141859a1f1f","sha256:5c5d0db58b58f3312b1fa405c777f40f76156af3465c66b2abb4f774ccb96e12"],"state_sha256":"11c085a5630d1892362cafbac315b598494639f9c607063f18f2aad6ff6ca68c"}