{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:UT4MKVLKOSS7TXOE43EOQAXKBR","short_pith_number":"pith:UT4MKVLK","schema_version":"1.0","canonical_sha256":"a4f8c5556a74a5f9ddc4e6c8e802ea0c60d1918e5eff5a2cf287c851f82562fa","source":{"kind":"arxiv","id":"1901.00574","version":1},"attestation_state":"computed","paper":{"title":"Measurement of the Stark shift of the $6s^2S_{1/2} \\rightarrow 7p^2P_{J} $ transitions in atomic cesium","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"D. Antypas, D. S. Elliott, George Toh","submitted_at":"2019-01-03T01:48:14Z","abstract_excerpt":"We report measurements of the Stark shift of the cesium $6s \\: ^2S_{3/2} \\rightarrow 7p \\: ^2P_{3/2} $ and the $6s \\: ^2S_{1/2} \\rightarrow 7p \\: ^2P_{1/2} $ transitions at $\\lambda = 456$ nm and 459 nm, respectively, in an atomic beam. From these, we determine the static scalar polarizability for both 7P states, and the tensor polarizability for the 7P$_{3/2}$ state. The fractional uncertainty of the scalar polarizabilites is $\\sim$0.18\\%, while that of the tensor term is 0.66\\%. These measurements provide sensitive tests of theoretical models of the Cs atom, which has played a central role i"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1901.00574","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2019-01-03T01:48:14Z","cross_cats_sorted":[],"title_canon_sha256":"fa21687fa26438f06ddc0488910abbf8c54345a692209f95c090a656e50c3a33","abstract_canon_sha256":"1d72c5e5a5433c9012644fb4065d11d5a6c6c65827a7a31cd89e65adf2b5623c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:57:02.108108Z","signature_b64":"TwuBruqCFnEk0qF+Gkkjnu0WONKEihk6D8AM0uo005WeMSBdv8BTQBeQCdmg81f1Vqop9kOJkooURK/SWQL1DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a4f8c5556a74a5f9ddc4e6c8e802ea0c60d1918e5eff5a2cf287c851f82562fa","last_reissued_at":"2026-05-17T23:57:02.107610Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:57:02.107610Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of the Stark shift of the $6s^2S_{1/2} \\rightarrow 7p^2P_{J} $ transitions in atomic cesium","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"D. Antypas, D. S. Elliott, George Toh","submitted_at":"2019-01-03T01:48:14Z","abstract_excerpt":"We report measurements of the Stark shift of the cesium $6s \\: ^2S_{3/2} \\rightarrow 7p \\: ^2P_{3/2} $ and the $6s \\: ^2S_{1/2} \\rightarrow 7p \\: ^2P_{1/2} $ transitions at $\\lambda = 456$ nm and 459 nm, respectively, in an atomic beam. From these, we determine the static scalar polarizability for both 7P states, and the tensor polarizability for the 7P$_{3/2}$ state. The fractional uncertainty of the scalar polarizabilites is $\\sim$0.18\\%, while that of the tensor term is 0.66\\%. These measurements provide sensitive tests of theoretical models of the Cs atom, which has played a central role i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.00574","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1901.00574","created_at":"2026-05-17T23:57:02.107695+00:00"},{"alias_kind":"arxiv_version","alias_value":"1901.00574v1","created_at":"2026-05-17T23:57:02.107695+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.00574","created_at":"2026-05-17T23:57:02.107695+00:00"},{"alias_kind":"pith_short_12","alias_value":"UT4MKVLKOSS7","created_at":"2026-05-18T12:33:30.264802+00:00"},{"alias_kind":"pith_short_16","alias_value":"UT4MKVLKOSS7TXOE","created_at":"2026-05-18T12:33:30.264802+00:00"},{"alias_kind":"pith_short_8","alias_value":"UT4MKVLK","created_at":"2026-05-18T12:33:30.264802+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UT4MKVLKOSS7TXOE43EOQAXKBR","json":"https://pith.science/pith/UT4MKVLKOSS7TXOE43EOQAXKBR.json","graph_json":"https://pith.science/api/pith-number/UT4MKVLKOSS7TXOE43EOQAXKBR/graph.json","events_json":"https://pith.science/api/pith-number/UT4MKVLKOSS7TXOE43EOQAXKBR/events.json","paper":"https://pith.science/paper/UT4MKVLK"},"agent_actions":{"view_html":"https://pith.science/pith/UT4MKVLKOSS7TXOE43EOQAXKBR","download_json":"https://pith.science/pith/UT4MKVLKOSS7TXOE43EOQAXKBR.json","view_paper":"https://pith.science/paper/UT4MKVLK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1901.00574&json=true","fetch_graph":"https://pith.science/api/pith-number/UT4MKVLKOSS7TXOE43EOQAXKBR/graph.json","fetch_events":"https://pith.science/api/pith-number/UT4MKVLKOSS7TXOE43EOQAXKBR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UT4MKVLKOSS7TXOE43EOQAXKBR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UT4MKVLKOSS7TXOE43EOQAXKBR/action/storage_attestation","attest_author":"https://pith.science/pith/UT4MKVLKOSS7TXOE43EOQAXKBR/action/author_attestation","sign_citation":"https://pith.science/pith/UT4MKVLKOSS7TXOE43EOQAXKBR/action/citation_signature","submit_replication":"https://pith.science/pith/UT4MKVLKOSS7TXOE43EOQAXKBR/action/replication_record"}},"created_at":"2026-05-17T23:57:02.107695+00:00","updated_at":"2026-05-17T23:57:02.107695+00:00"}