{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:WWR4KWOFUGM2H3DB46ORUJO4NC","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":"2e80189641edf88918a5b3bb15ccc8d38e215e33ef494513f504173ef639ef19","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-01-02T18:30:20Z","title_canon_sha256":"8d7486b37cac82889b7d69be5356f39345dcec6dbbe39394c9b70525f688e339"},"schema_version":"1.0","source":{"id":"1901.00480","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1901.00480","created_at":"2026-05-17T23:51:30Z"},{"alias_kind":"arxiv_version","alias_value":"1901.00480v1","created_at":"2026-05-17T23:51:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.00480","created_at":"2026-05-17T23:51:30Z"},{"alias_kind":"pith_short_12","alias_value":"WWR4KWOFUGM2","created_at":"2026-05-18T12:33:33Z"},{"alias_kind":"pith_short_16","alias_value":"WWR4KWOFUGM2H3DB","created_at":"2026-05-18T12:33:33Z"},{"alias_kind":"pith_short_8","alias_value":"WWR4KWOF","created_at":"2026-05-18T12:33:33Z"}],"graph_snapshots":[{"event_id":"sha256:ac28834990e23a7e272d3c7440f1e5444638c714150049c1362a942ddc95c355","target":"graph","created_at":"2026-05-17T23:51:30Z","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 a measurement of the ratio of electric dipole transition matrix elements of cesium for the $6p\\,^2P_{1/2} \\rightarrow 7s\\,^2S_{1/2}$ and $6p\\,^2P_{3/2} \\rightarrow 7s\\,^2S_{1/2}$ transitions. We determine this ratio of matrix elements through comparisons of two-color, two-photon excitation rates of the $7s\\,^2S_{1/2}$ state using laser beams with polarizations parallel to one another vs.\\ perpendicular to one another. Our result of $R \\equiv \\langle 7s\\ ^2S_{1/2} || r || 6p\\ ^2P_{3/2} \\rangle / \\langle 7s\\ ^2S_{1/2} || r || 6p\\ ^2P_{1/2} \\rangle = 1.5272 \\ (17)$ is in excellent agree","authors_text":"Amy Damitz, D. S. Elliott, George Toh, I. C. Stevenson, J. Choi, Jonah Quirk, M. S. Safronova, Nathan Glotzbach","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-01-02T18:30:20Z","title":"Electric dipole matrix elements for the $6p\\ ^2P_J \\rightarrow 7s\\ ^2S_{1/2}$ transition in atomic cesium"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.00480","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":"sha256:6f36d9eac881c096fc463f8e92317fec97898bf5df764b76ecb99afdbb3f265e","target":"record","created_at":"2026-05-17T23:51:30Z","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":"2e80189641edf88918a5b3bb15ccc8d38e215e33ef494513f504173ef639ef19","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-01-02T18:30:20Z","title_canon_sha256":"8d7486b37cac82889b7d69be5356f39345dcec6dbbe39394c9b70525f688e339"},"schema_version":"1.0","source":{"id":"1901.00480","kind":"arxiv","version":1}},"canonical_sha256":"b5a3c559c5a199a3ec61e79d1a25dc689ab9a6e61076510be1c5d62e1dfa492a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b5a3c559c5a199a3ec61e79d1a25dc689ab9a6e61076510be1c5d62e1dfa492a","first_computed_at":"2026-05-17T23:51:30.365675Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:51:30.365675Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"+f0R/3FbEiVIMYQ3KWcD/GFRaSnZVHcFe0wWbCN8j95UO1Hgo9juNFw6r0qdHBJPXgZToAcFMD4kD9tlF8b2Bw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:51:30.366219Z","signed_message":"canonical_sha256_bytes"},"source_id":"1901.00480","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6f36d9eac881c096fc463f8e92317fec97898bf5df764b76ecb99afdbb3f265e","sha256:ac28834990e23a7e272d3c7440f1e5444638c714150049c1362a942ddc95c355"],"state_sha256":"fed9d062945a23ffd0fdc19d5011a8264cac5ebb7e89696d171c81b5d8a29eba"}