{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:LFIYZFPMRIDBVVXQZN74XVTR4D","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":"3659d8254f8ed480388c2514d65175f3b0460deabf9222c7bdf2082cb01c4595","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-04-12T18:02:29Z","title_canon_sha256":"4e9c8b62dca90971a2291f341d5c8ea9ac2ee63569c8509adac4f231e06e4144"},"schema_version":"1.0","source":{"id":"1904.06362","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1904.06362","created_at":"2026-05-17T23:42:19Z"},{"alias_kind":"arxiv_version","alias_value":"1904.06362v1","created_at":"2026-05-17T23:42:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1904.06362","created_at":"2026-05-17T23:42:19Z"},{"alias_kind":"pith_short_12","alias_value":"LFIYZFPMRIDB","created_at":"2026-05-18T12:33:21Z"},{"alias_kind":"pith_short_16","alias_value":"LFIYZFPMRIDBVVXQ","created_at":"2026-05-18T12:33:21Z"},{"alias_kind":"pith_short_8","alias_value":"LFIYZFPM","created_at":"2026-05-18T12:33:21Z"}],"graph_snapshots":[{"event_id":"sha256:b741d8322a9a7044dd73d9c9411042a0c36a608e758b4b467f9a54f3846cd1bf","target":"graph","created_at":"2026-05-17T23:42:19Z","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":"We report measurements of the electric dipole matrix elements of the $^{133}$Cs $\\ $ $6s\\,^2S_{1/2} \\rightarrow 7p\\,^2P_{1/2}$ and $6s\\,^2S_{1/2} \\rightarrow 7p\\,^2P_{3/2}$ transitions. Each of these determinations is based on direct, precise comparisons of the absorption coefficients between two absorption lines. For the $\\langle 6s\\,^2S_{1/2}||r|| 7p\\,^2P_{3/2} \\rangle$ matrix element, we measure the ratio of the absorption coefficient on this line with that of the D$_1$ transition, $6s\\,^2S_{1/2} \\rightarrow 6p\\,^2P_{1/2}$. The matrix element of the D$_1$ line has been determined with high ","authors_text":"Amy Damitz, Carol E. Tanner, D. S. Elliott, Eric Putney, George Toh","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-04-12T18:02:29Z","title":"Measurement of the radial matrix elements for the $6s ^2S_{1/2} \\rightarrow 7p ^2P_J$ transitions in cesium"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1904.06362","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:ddf885207229629fc97ca57a8a0a5e6e556619208312836baa88b75b9fc0997a","target":"record","created_at":"2026-05-17T23:42:19Z","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":"3659d8254f8ed480388c2514d65175f3b0460deabf9222c7bdf2082cb01c4595","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-04-12T18:02:29Z","title_canon_sha256":"4e9c8b62dca90971a2291f341d5c8ea9ac2ee63569c8509adac4f231e06e4144"},"schema_version":"1.0","source":{"id":"1904.06362","kind":"arxiv","version":1}},"canonical_sha256":"59518c95ec8a061ad6f0cb7fcbd671e0f3d4ab343a2077fe45ab3acec13d2337","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"59518c95ec8a061ad6f0cb7fcbd671e0f3d4ab343a2077fe45ab3acec13d2337","first_computed_at":"2026-05-17T23:42:19.847847Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:42:19.847847Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wEpSg7I4/yMT0kh+7xv3pdOgtjjfq5gK7Q2j/cG/DmwTgxU5BaBBVyhK6BqO0deKYjVnnWOuEutC0c37BMqMBw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:42:19.848255Z","signed_message":"canonical_sha256_bytes"},"source_id":"1904.06362","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ddf885207229629fc97ca57a8a0a5e6e556619208312836baa88b75b9fc0997a","sha256:b741d8322a9a7044dd73d9c9411042a0c36a608e758b4b467f9a54f3846cd1bf"],"state_sha256":"078d44a672c75bda1ae810eec50290b20925f03bba5a23929d4a655f73cd13ac"}