{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:LXZQABVNJYSCBAORLW4V3LSC4Z","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":"b22e8ec98a048b78cd7b52ccc03ad9e2e2c02405205023b8f581085b8dc18613","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-09-04T14:20:21Z","title_canon_sha256":"161d18aa8d75d72ee55b6ff9c74597185f01a0ab0e87ec03a8a88d98740cc2a5"},"schema_version":"1.0","source":{"id":"1909.01991","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1909.01991","created_at":"2026-07-05T00:02:29Z"},{"alias_kind":"arxiv_version","alias_value":"1909.01991v1","created_at":"2026-07-05T00:02:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1909.01991","created_at":"2026-07-05T00:02:29Z"},{"alias_kind":"pith_short_12","alias_value":"LXZQABVNJYSC","created_at":"2026-07-05T00:02:29Z"},{"alias_kind":"pith_short_16","alias_value":"LXZQABVNJYSCBAOR","created_at":"2026-07-05T00:02:29Z"},{"alias_kind":"pith_short_8","alias_value":"LXZQABVN","created_at":"2026-07-05T00:02:29Z"}],"graph_snapshots":[{"event_id":"sha256:c73192ed90ca628ae824455f38adf901837b586ad767e6c08d10f8d58eba0fdc","target":"graph","created_at":"2026-07-05T00:02:29Z","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/1909.01991/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We report new precision measurements of the $^{20}$Ne--$^{22}$Ne isotope shift for several transitions, as well as state-of-the-art, \\textit{ab initio} field-shift calculations. Our results are combined with historical measurements in a global fit to obtain the isotope shifts of all fifty low-lying neon levels with high precision. These level shifts show a wealth of electronic, nuclear, and relativistic phenomena. Relying on the analogy between mass shift and fine-structure operators, we explain this plethora of neon level-shifts utilizing a small number of effective parameters in a global par","authors_text":"A. J. Geddes, B. Ohayon, G. Ron, H. Rahangdale, J. C. Berengut","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-09-04T14:20:21Z","title":"Isotope shifts in $^{20,22}$Ne -- Precision measurements and global analysis in the framework of intermediate coupling"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1909.01991","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":"sha256:1030afe3f323d1e92b4df5a424b89cb00349d6f3f99de00eb47dd45fd8f8b741","target":"record","created_at":"2026-07-05T00:02:29Z","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":"b22e8ec98a048b78cd7b52ccc03ad9e2e2c02405205023b8f581085b8dc18613","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-09-04T14:20:21Z","title_canon_sha256":"161d18aa8d75d72ee55b6ff9c74597185f01a0ab0e87ec03a8a88d98740cc2a5"},"schema_version":"1.0","source":{"id":"1909.01991","kind":"arxiv","version":1}},"canonical_sha256":"5df30006ad4e242081d15db95dae42e64d1dcd98d14d72f3637e2855288b4d15","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5df30006ad4e242081d15db95dae42e64d1dcd98d14d72f3637e2855288b4d15","first_computed_at":"2026-07-05T00:02:29.442161Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:02:29.442161Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nJvjeZJ9abBYPDuBOr5Ce0gffIb9miMb2GOTSEYNtlnU3EnyXvxenUlBxfFeYDJw+rBmVuTS7Cw7W3S3JzfXCA==","signature_status":"signed_v1","signed_at":"2026-07-05T00:02:29.442649Z","signed_message":"canonical_sha256_bytes"},"source_id":"1909.01991","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1030afe3f323d1e92b4df5a424b89cb00349d6f3f99de00eb47dd45fd8f8b741","sha256:c73192ed90ca628ae824455f38adf901837b586ad767e6c08d10f8d58eba0fdc"],"state_sha256":"2bbd95a9aa10e51ecb9927f87a0ca864cf5f9d9d6c0eaf554b6e497640ba1dbb"}