{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:CBV5L7DEAFFV7CEDSHLI3D3ITY","short_pith_number":"pith:CBV5L7DE","schema_version":"1.0","canonical_sha256":"106bd5fc64014b5f888391d68d8f689e065f51d962e1aa4c13ba83ff8b8293f3","source":{"kind":"arxiv","id":"1509.07091","version":2},"attestation_state":"computed","paper":{"title":"Measurements of the Ground-State Polarizabilities of Cs, Rb, and K using Atom Interferometry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Alexander D. Cronin, Ivan Hromada, Maxwell D. Gregoire, Raisa Trubko, William F. Holmgren","submitted_at":"2015-09-23T18:45:40Z","abstract_excerpt":"We measured the ground-state static electric-dipole polarizabilities of Cs, Rb, and K atoms using a three-nanograting Mach-Zehnder atom beam interferometer. Our measurements provide benchmark tests for atomic structure calculations and thus test the underlying theory used to interpret atomic parity non-conservation experiments. We measured $\\alpha_{\\mathrm{Cs}} = 4\\pi\\epsilon_0 \\times 59.45(11) \\AA^3$, $\\alpha_{\\mathrm{Rb}} = 4\\pi\\epsilon_0 \\times 47.44(9) \\AA^3$, and $\\alpha_{\\mathrm{K}} = 4\\pi\\epsilon_0 \\times 42.97(8) \\AA^3$. In atomic units, these measurements are $\\alpha_{\\mathrm{Cs}} = 4"},"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":"1509.07091","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-09-23T18:45:40Z","cross_cats_sorted":[],"title_canon_sha256":"3b7bc7ee01be918a757c4b15868626ef42800f6839fce209418998346a7bfa37","abstract_canon_sha256":"fd18ed03c4297ea5e6305a9e46c4ed3ecdf7e351cfed941f83a38047b0527695"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:26:09.508650Z","signature_b64":"AdhH3v0kNRs9SCbLx/1nXajkHGLHHu9NZYP7ZjPZnrW+d/YfZmYbU7BSh2JrveXgFVxLoNUvTdghuz80DnvDAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"106bd5fc64014b5f888391d68d8f689e065f51d962e1aa4c13ba83ff8b8293f3","last_reissued_at":"2026-05-18T01:26:09.508199Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:26:09.508199Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurements of the Ground-State Polarizabilities of Cs, Rb, and K using Atom Interferometry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Alexander D. Cronin, Ivan Hromada, Maxwell D. Gregoire, Raisa Trubko, William F. Holmgren","submitted_at":"2015-09-23T18:45:40Z","abstract_excerpt":"We measured the ground-state static electric-dipole polarizabilities of Cs, Rb, and K atoms using a three-nanograting Mach-Zehnder atom beam interferometer. Our measurements provide benchmark tests for atomic structure calculations and thus test the underlying theory used to interpret atomic parity non-conservation experiments. We measured $\\alpha_{\\mathrm{Cs}} = 4\\pi\\epsilon_0 \\times 59.45(11) \\AA^3$, $\\alpha_{\\mathrm{Rb}} = 4\\pi\\epsilon_0 \\times 47.44(9) \\AA^3$, and $\\alpha_{\\mathrm{K}} = 4\\pi\\epsilon_0 \\times 42.97(8) \\AA^3$. In atomic units, these measurements are $\\alpha_{\\mathrm{Cs}} = 4"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.07091","kind":"arxiv","version":2},"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":"1509.07091","created_at":"2026-05-18T01:26:09.508260+00:00"},{"alias_kind":"arxiv_version","alias_value":"1509.07091v2","created_at":"2026-05-18T01:26:09.508260+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.07091","created_at":"2026-05-18T01:26:09.508260+00:00"},{"alias_kind":"pith_short_12","alias_value":"CBV5L7DEAFFV","created_at":"2026-05-18T12:29:14.074870+00:00"},{"alias_kind":"pith_short_16","alias_value":"CBV5L7DEAFFV7CED","created_at":"2026-05-18T12:29:14.074870+00:00"},{"alias_kind":"pith_short_8","alias_value":"CBV5L7DE","created_at":"2026-05-18T12:29:14.074870+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/CBV5L7DEAFFV7CEDSHLI3D3ITY","json":"https://pith.science/pith/CBV5L7DEAFFV7CEDSHLI3D3ITY.json","graph_json":"https://pith.science/api/pith-number/CBV5L7DEAFFV7CEDSHLI3D3ITY/graph.json","events_json":"https://pith.science/api/pith-number/CBV5L7DEAFFV7CEDSHLI3D3ITY/events.json","paper":"https://pith.science/paper/CBV5L7DE"},"agent_actions":{"view_html":"https://pith.science/pith/CBV5L7DEAFFV7CEDSHLI3D3ITY","download_json":"https://pith.science/pith/CBV5L7DEAFFV7CEDSHLI3D3ITY.json","view_paper":"https://pith.science/paper/CBV5L7DE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1509.07091&json=true","fetch_graph":"https://pith.science/api/pith-number/CBV5L7DEAFFV7CEDSHLI3D3ITY/graph.json","fetch_events":"https://pith.science/api/pith-number/CBV5L7DEAFFV7CEDSHLI3D3ITY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CBV5L7DEAFFV7CEDSHLI3D3ITY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CBV5L7DEAFFV7CEDSHLI3D3ITY/action/storage_attestation","attest_author":"https://pith.science/pith/CBV5L7DEAFFV7CEDSHLI3D3ITY/action/author_attestation","sign_citation":"https://pith.science/pith/CBV5L7DEAFFV7CEDSHLI3D3ITY/action/citation_signature","submit_replication":"https://pith.science/pith/CBV5L7DEAFFV7CEDSHLI3D3ITY/action/replication_record"}},"created_at":"2026-05-18T01:26:09.508260+00:00","updated_at":"2026-05-18T01:26:09.508260+00:00"}