{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:W223KHXU2AVGP32ULINNQ6YLG5","short_pith_number":"pith:W223KHXU","schema_version":"1.0","canonical_sha256":"b6b5b51ef4d02a67ef545a1ad87b0b37404a892bde0662a7826d8d9dd6ca2ef1","source":{"kind":"arxiv","id":"0906.0571","version":1},"attestation_state":"computed","paper":{"title":"Electromagnetically Induced Transparency versus Nonlinear Faraday Effect. Coherent Control of the Light Beam Polarization","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"physics.optics","authors_text":"R. Drampyan, S. Pustelny, W. Gawlik","submitted_at":"2009-06-02T22:23:21Z","abstract_excerpt":"We report on experimental and theoretical study of the nonlinear Faraday effect under conditions of electromagnetically induced transparency at the 5$S_{1/2} \\to 5P_{3/2} \\to 5D_{5/2}$ two-photon transition in rubidium vapors. These transitions realize the inverted Y model which combines the $\\Lambda$ and ladder systems. Strong nonlinearity allowing for large rotation angles of a probe beam tuned to the $S\\to P$ transition was obtained by creation of quantum superpositions of magnetic sublevels (Zeeman coherences) in the rubidium ground state ($\\Lambda$ scheme). Additionally, electromagnetical"},"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":"0906.0571","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2009-06-02T22:23:21Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"ba8d44acfe89d7d9f24734ea11d71d6adf8b83eb93b558d3e13939acb4019a62","abstract_canon_sha256":"bf1c25e5c0493dbb8814b23a17e3dd2cc8f4e70df39bf2dfab767f9c3c51aa84"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:13:29.603007Z","signature_b64":"PThZi89mhglcfaR3ACRpycLAI6lB8UccsVh7eQHCzdQ+R7WCt8NzOL5R8mYI6klAHokvL1Hmc4Tmyy1KUJMRBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b6b5b51ef4d02a67ef545a1ad87b0b37404a892bde0662a7826d8d9dd6ca2ef1","last_reissued_at":"2026-05-18T02:13:29.602392Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:13:29.602392Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electromagnetically Induced Transparency versus Nonlinear Faraday Effect. Coherent Control of the Light Beam Polarization","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"physics.optics","authors_text":"R. Drampyan, S. Pustelny, W. Gawlik","submitted_at":"2009-06-02T22:23:21Z","abstract_excerpt":"We report on experimental and theoretical study of the nonlinear Faraday effect under conditions of electromagnetically induced transparency at the 5$S_{1/2} \\to 5P_{3/2} \\to 5D_{5/2}$ two-photon transition in rubidium vapors. These transitions realize the inverted Y model which combines the $\\Lambda$ and ladder systems. Strong nonlinearity allowing for large rotation angles of a probe beam tuned to the $S\\to P$ transition was obtained by creation of quantum superpositions of magnetic sublevels (Zeeman coherences) in the rubidium ground state ($\\Lambda$ scheme). Additionally, electromagnetical"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0906.0571","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":"0906.0571","created_at":"2026-05-18T02:13:29.602476+00:00"},{"alias_kind":"arxiv_version","alias_value":"0906.0571v1","created_at":"2026-05-18T02:13:29.602476+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0906.0571","created_at":"2026-05-18T02:13:29.602476+00:00"},{"alias_kind":"pith_short_12","alias_value":"W223KHXU2AVG","created_at":"2026-05-18T12:26:02.257875+00:00"},{"alias_kind":"pith_short_16","alias_value":"W223KHXU2AVGP32U","created_at":"2026-05-18T12:26:02.257875+00:00"},{"alias_kind":"pith_short_8","alias_value":"W223KHXU","created_at":"2026-05-18T12:26:02.257875+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/W223KHXU2AVGP32ULINNQ6YLG5","json":"https://pith.science/pith/W223KHXU2AVGP32ULINNQ6YLG5.json","graph_json":"https://pith.science/api/pith-number/W223KHXU2AVGP32ULINNQ6YLG5/graph.json","events_json":"https://pith.science/api/pith-number/W223KHXU2AVGP32ULINNQ6YLG5/events.json","paper":"https://pith.science/paper/W223KHXU"},"agent_actions":{"view_html":"https://pith.science/pith/W223KHXU2AVGP32ULINNQ6YLG5","download_json":"https://pith.science/pith/W223KHXU2AVGP32ULINNQ6YLG5.json","view_paper":"https://pith.science/paper/W223KHXU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0906.0571&json=true","fetch_graph":"https://pith.science/api/pith-number/W223KHXU2AVGP32ULINNQ6YLG5/graph.json","fetch_events":"https://pith.science/api/pith-number/W223KHXU2AVGP32ULINNQ6YLG5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W223KHXU2AVGP32ULINNQ6YLG5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W223KHXU2AVGP32ULINNQ6YLG5/action/storage_attestation","attest_author":"https://pith.science/pith/W223KHXU2AVGP32ULINNQ6YLG5/action/author_attestation","sign_citation":"https://pith.science/pith/W223KHXU2AVGP32ULINNQ6YLG5/action/citation_signature","submit_replication":"https://pith.science/pith/W223KHXU2AVGP32ULINNQ6YLG5/action/replication_record"}},"created_at":"2026-05-18T02:13:29.602476+00:00","updated_at":"2026-05-18T02:13:29.602476+00:00"}