{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:Q34OWJ3YP66OPRGIIDJCACLTJP","short_pith_number":"pith:Q34OWJ3Y","schema_version":"1.0","canonical_sha256":"86f8eb27787fbce7c4c840d22009734bf21d5e0fc7f6d1fa7f159a098a728c30","source":{"kind":"arxiv","id":"1410.8171","version":2},"attestation_state":"computed","paper":{"title":"Controlling the magnetic field sensitivity of atomic clock states by microwave dressing","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas"],"primary_cat":"physics.atom-ph","authors_text":"H. Hattermann, J. Fort\\'agh, L. S\\'ark\\'any, P. Weiss","submitted_at":"2014-10-29T21:25:51Z","abstract_excerpt":"We demonstrate control of the differential Zeeman shift between clock states of ultracold rubidium atoms by means of non-resonant microwave dressing. Using the dc-field dependence of the microwave detuning, we suppress the first and second order differential Zeeman shift in magnetically trapped $^{87}$Rb atoms. By dressing the state pair 5S$_{1/2} F= 1, m_F = -1$ and $F= 2, m_F = 1$, a residual frequency spread of <0.1 Hz in a range of 100 mG around a chosen magnetic offset field can be achieved. This is one order of magnitude smaller than the shift of the bare states at the magic field of the"},"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":"1410.8171","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-10-29T21:25:51Z","cross_cats_sorted":["cond-mat.quant-gas"],"title_canon_sha256":"c34ffd248cc047c951c7be184e379dbd0aab35febeac3457345b3b08ac7ae23a","abstract_canon_sha256":"ec17f0a02195d867ebc6bd9c2d318cc389c18ae484e678bc44169379363fa792"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:29.003890Z","signature_b64":"34xIZi1o1VGHqmGsswvG0kwNf1q7ZvOJTFtlgyse/X42ucoycxD2BUgNidlJTu+EuGp9IyWLPUBrpWeBssDvCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"86f8eb27787fbce7c4c840d22009734bf21d5e0fc7f6d1fa7f159a098a728c30","last_reissued_at":"2026-05-18T00:40:29.003358Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:29.003358Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Controlling the magnetic field sensitivity of atomic clock states by microwave dressing","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas"],"primary_cat":"physics.atom-ph","authors_text":"H. Hattermann, J. Fort\\'agh, L. S\\'ark\\'any, P. Weiss","submitted_at":"2014-10-29T21:25:51Z","abstract_excerpt":"We demonstrate control of the differential Zeeman shift between clock states of ultracold rubidium atoms by means of non-resonant microwave dressing. Using the dc-field dependence of the microwave detuning, we suppress the first and second order differential Zeeman shift in magnetically trapped $^{87}$Rb atoms. By dressing the state pair 5S$_{1/2} F= 1, m_F = -1$ and $F= 2, m_F = 1$, a residual frequency spread of <0.1 Hz in a range of 100 mG around a chosen magnetic offset field can be achieved. This is one order of magnitude smaller than the shift of the bare states at the magic field of the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.8171","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":"1410.8171","created_at":"2026-05-18T00:40:29.003444+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.8171v2","created_at":"2026-05-18T00:40:29.003444+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.8171","created_at":"2026-05-18T00:40:29.003444+00:00"},{"alias_kind":"pith_short_12","alias_value":"Q34OWJ3YP66O","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_16","alias_value":"Q34OWJ3YP66OPRGI","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_8","alias_value":"Q34OWJ3Y","created_at":"2026-05-18T12:28:43.426989+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/Q34OWJ3YP66OPRGIIDJCACLTJP","json":"https://pith.science/pith/Q34OWJ3YP66OPRGIIDJCACLTJP.json","graph_json":"https://pith.science/api/pith-number/Q34OWJ3YP66OPRGIIDJCACLTJP/graph.json","events_json":"https://pith.science/api/pith-number/Q34OWJ3YP66OPRGIIDJCACLTJP/events.json","paper":"https://pith.science/paper/Q34OWJ3Y"},"agent_actions":{"view_html":"https://pith.science/pith/Q34OWJ3YP66OPRGIIDJCACLTJP","download_json":"https://pith.science/pith/Q34OWJ3YP66OPRGIIDJCACLTJP.json","view_paper":"https://pith.science/paper/Q34OWJ3Y","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.8171&json=true","fetch_graph":"https://pith.science/api/pith-number/Q34OWJ3YP66OPRGIIDJCACLTJP/graph.json","fetch_events":"https://pith.science/api/pith-number/Q34OWJ3YP66OPRGIIDJCACLTJP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Q34OWJ3YP66OPRGIIDJCACLTJP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Q34OWJ3YP66OPRGIIDJCACLTJP/action/storage_attestation","attest_author":"https://pith.science/pith/Q34OWJ3YP66OPRGIIDJCACLTJP/action/author_attestation","sign_citation":"https://pith.science/pith/Q34OWJ3YP66OPRGIIDJCACLTJP/action/citation_signature","submit_replication":"https://pith.science/pith/Q34OWJ3YP66OPRGIIDJCACLTJP/action/replication_record"}},"created_at":"2026-05-18T00:40:29.003444+00:00","updated_at":"2026-05-18T00:40:29.003444+00:00"}