{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:BCIQFOIJRTC2COS3SVQ2SGRI5S","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":"8480f11a0c3ad6c60c3e374b53b5f5247a6e753f74b9bdc812fbeed98f7e475e","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-06-13T15:02:19Z","title_canon_sha256":"b8b9f57877aa51daec648078e9f334a7e9d00b3b7856eb93ad54c3c0de8377dc"},"schema_version":"1.0","source":{"id":"1406.3560","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.3560","created_at":"2026-05-18T01:01:29Z"},{"alias_kind":"arxiv_version","alias_value":"1406.3560v3","created_at":"2026-05-18T01:01:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.3560","created_at":"2026-05-18T01:01:29Z"},{"alias_kind":"pith_short_12","alias_value":"BCIQFOIJRTC2","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"BCIQFOIJRTC2COS3","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"BCIQFOIJ","created_at":"2026-05-18T12:28:22Z"}],"graph_snapshots":[{"event_id":"sha256:f2b1a56fa7cb71af5108185620fffce65434d1ff0a7280db8263963281e2a214","target":"graph","created_at":"2026-05-18T01:01:29Z","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 analyze doubly magic trapping of Cs hyperfine transitions including previously neglected contributions from the ground state hyperpolarizability and the interaction of the laser light and a static magnetic field. Extensive numerical searches do not reveal any doubly magic trapping conditions for any pair of hyperfine states. However, including the hyperpolarizability reveals light intensity insensitive traps for a wide range of wavelengths at specific intensities. We then investigate the possibility of using bichromatic trapping light fields. Deploying a bichromatic scheme, we demonstrate d","authors_text":"A. W. Carr, M. Saffman","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-06-13T15:02:19Z","title":"Doubly magic optical trapping for Cs atom hyperfine clock transitions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.3560","kind":"arxiv","version":3},"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":"sha256:3b9ffab817fdab6d5a3eecd2060fa2f15a45274b9b8309a71774ad207f434fb4","target":"record","created_at":"2026-05-18T01:01:29Z","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":"8480f11a0c3ad6c60c3e374b53b5f5247a6e753f74b9bdc812fbeed98f7e475e","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-06-13T15:02:19Z","title_canon_sha256":"b8b9f57877aa51daec648078e9f334a7e9d00b3b7856eb93ad54c3c0de8377dc"},"schema_version":"1.0","source":{"id":"1406.3560","kind":"arxiv","version":3}},"canonical_sha256":"089102b9098cc5a13a5b9561a91a28ec9a391175d9c116e66d1ba97c1fd85040","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"089102b9098cc5a13a5b9561a91a28ec9a391175d9c116e66d1ba97c1fd85040","first_computed_at":"2026-05-18T01:01:29.488783Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:01:29.488783Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"r+YXOXzLe3X3qdE2HbqWQHqGCGdhGRsVg+KaJ9Bg9I7RcEVdL+8Ixe4hlqZyTM/4FvugqAPANLWgW+NaEenEBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:01:29.489234Z","signed_message":"canonical_sha256_bytes"},"source_id":"1406.3560","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3b9ffab817fdab6d5a3eecd2060fa2f15a45274b9b8309a71774ad207f434fb4","sha256:f2b1a56fa7cb71af5108185620fffce65434d1ff0a7280db8263963281e2a214"],"state_sha256":"5875155b2d13560f2421d9db8e6aac90d8a7386a68b7b7c05bf30008edf1158e"}