{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:DD3CIA5KAU7TD5CWUBJHS6QI6N","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":"322e4c2e9eeff1b9a16c5d3c12d3e89516677794f495ec116efe497f70037e62","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-07-11T02:57:44Z","title_canon_sha256":"600f7d8cc4ccadf79451c70f0880282c402ce85631a9eb6003e66f0cdb9ee476"},"schema_version":"1.0","source":{"id":"2507.08278","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2507.08278","created_at":"2026-07-05T11:35:20Z"},{"alias_kind":"arxiv_version","alias_value":"2507.08278v1","created_at":"2026-07-05T11:35:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.08278","created_at":"2026-07-05T11:35:20Z"},{"alias_kind":"pith_short_12","alias_value":"DD3CIA5KAU7T","created_at":"2026-07-05T11:35:20Z"},{"alias_kind":"pith_short_16","alias_value":"DD3CIA5KAU7TD5CW","created_at":"2026-07-05T11:35:20Z"},{"alias_kind":"pith_short_8","alias_value":"DD3CIA5K","created_at":"2026-07-05T11:35:20Z"}],"graph_snapshots":[{"event_id":"sha256:725474db876481080c1a9475c9b301ae1385bd7363fda60da1db6bb63a223a4a","target":"graph","created_at":"2026-07-05T11:35:20Z","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/2507.08278/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The response of an atom to external electric and magnetic fields can reveal fundamental atomic properties. It has long been verified that, in a static magnetic field, those atomic energy levels with hyperfine interactions shift according to the Breit-Rabi formula, which introduces nonlinear dependence on the magnetic field. On the other hand, the corresponding Breit-Rabi dependence on a static electric field has not been observed before due to a combination of experimental challenges. Here we precisely measure the Stark shift of the $6s^2\\ ^1S_0\\ \\leftrightarrow\\ 6s6p\\ ^1P_1$ transition of $^{","authors_text":"S.-B. Wang, S.-Z. Wang, T. Xia, Z.-J. Tao, Z.-T. Lu","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-07-11T02:57:44Z","title":"Observation of the electric Breit-Rabi Effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.08278","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:d87ff0ae2737952447d182d1ed060e5eeef203b299accb8dbad1941e30442393","target":"record","created_at":"2026-07-05T11:35:20Z","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":"322e4c2e9eeff1b9a16c5d3c12d3e89516677794f495ec116efe497f70037e62","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-07-11T02:57:44Z","title_canon_sha256":"600f7d8cc4ccadf79451c70f0880282c402ce85631a9eb6003e66f0cdb9ee476"},"schema_version":"1.0","source":{"id":"2507.08278","kind":"arxiv","version":1}},"canonical_sha256":"18f62403aa053f31f456a052797a08f3763811d91350ccf3493f2620e7420830","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"18f62403aa053f31f456a052797a08f3763811d91350ccf3493f2620e7420830","first_computed_at":"2026-07-05T11:35:20.551421Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:35:20.551421Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AK0izWDpF6KL2k4D5/jNRKHRFLuVrRjFuFYvZNoswsxbCJ6ywuHoKhnUYb9BLPUzYrCyl3OFoNrBB90dLpn0CQ==","signature_status":"signed_v1","signed_at":"2026-07-05T11:35:20.551963Z","signed_message":"canonical_sha256_bytes"},"source_id":"2507.08278","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d87ff0ae2737952447d182d1ed060e5eeef203b299accb8dbad1941e30442393","sha256:725474db876481080c1a9475c9b301ae1385bd7363fda60da1db6bb63a223a4a"],"state_sha256":"4fbddc9ec3af66dd9a213db1d775ef332f7934645ad25f5a7be6a7f1a34f74cc"}