{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:ZALDXM3PTTGHLLXSOVACFYRRRB","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":"f39e8c1a28ca589ff2b9eec350b4d6f64c9223421fdedaff1967fd0c6cd7a058","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-03-23T15:43:45Z","title_canon_sha256":"9ed1c625aedb65130dbf37ba2c34349c3ca4a17454e689adc362c98f06ee1568"},"schema_version":"1.0","source":{"id":"2603.22119","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2603.22119","created_at":"2026-05-29T02:05:43Z"},{"alias_kind":"arxiv_version","alias_value":"2603.22119v2","created_at":"2026-05-29T02:05:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.22119","created_at":"2026-05-29T02:05:43Z"},{"alias_kind":"pith_short_12","alias_value":"ZALDXM3PTTGH","created_at":"2026-05-29T02:05:43Z"},{"alias_kind":"pith_short_16","alias_value":"ZALDXM3PTTGHLLXS","created_at":"2026-05-29T02:05:43Z"},{"alias_kind":"pith_short_8","alias_value":"ZALDXM3P","created_at":"2026-05-29T02:05:43Z"}],"graph_snapshots":[{"event_id":"sha256:8f74006474c5b292d7eea9a9abee9eb160ee678ad434be76a0f95cee1019f4eb","target":"graph","created_at":"2026-05-29T02:05:43Z","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/2603.22119/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The well-known graphical representation called the Lu-Fano plot was originally developed for multi-channel Rydberg spectroscopy, especially in quantum defect theory. The present study shows some of the limitations of this traditional Lu-Fano plot that are desirable to improve on, when there are closely split ionization thresholds as in many current generation quantum information applications involving hyperfine-split thresholds, or when there are more than two ionization threshold energies. The modified representation introduced here is especially simplifying in the situation where one is expl","authors_text":"Chris H. Greene, Justin D. Piel","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-03-23T15:43:45Z","title":"An alternative representation of multichannel Rydberg spectra: a modified K-matrix and Lu-Fano plot, applied to manganese spectroscopy"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.22119","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:c64562144cf25b2e9c054164edeb3b9ab02d083682fbcee25d2391f890c544d8","target":"record","created_at":"2026-05-29T02:05:43Z","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":"f39e8c1a28ca589ff2b9eec350b4d6f64c9223421fdedaff1967fd0c6cd7a058","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-03-23T15:43:45Z","title_canon_sha256":"9ed1c625aedb65130dbf37ba2c34349c3ca4a17454e689adc362c98f06ee1568"},"schema_version":"1.0","source":{"id":"2603.22119","kind":"arxiv","version":2}},"canonical_sha256":"c8163bb36f9ccc75aef2754022e23188760411824b8e6612537cbb83094a1970","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c8163bb36f9ccc75aef2754022e23188760411824b8e6612537cbb83094a1970","first_computed_at":"2026-05-29T02:05:43.443360Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-29T02:05:43.443360Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"P355d5s3qE7QzEMFgLq96jOm7Nr7AGybCKL6Oa0aiTjCbnKNqw1viBcmlmrqJ7RVqA7Ci5wfhFzOLWp4Nim3CA==","signature_status":"signed_v1","signed_at":"2026-05-29T02:05:43.444347Z","signed_message":"canonical_sha256_bytes"},"source_id":"2603.22119","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c64562144cf25b2e9c054164edeb3b9ab02d083682fbcee25d2391f890c544d8","sha256:8f74006474c5b292d7eea9a9abee9eb160ee678ad434be76a0f95cee1019f4eb"],"state_sha256":"fd807804a54e7f95abbe3ede215f82f8fa6c169b4f284608888d868831e76937"}