{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:BRDQW3OHTKSCSJW5YKRFSZEXSI","short_pith_number":"pith:BRDQW3OH","schema_version":"1.0","canonical_sha256":"0c470b6dc79aa42926ddc2a259649792134453998ccb1cd946f7f2167fdad79a","source":{"kind":"arxiv","id":"1502.07868","version":3},"attestation_state":"computed","paper":{"title":"Fluctuation properties of laser light after interaction with an atomic system: comparison between two-level and multilevel atomic transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"A. Kastberg, A. Lezama, R. Kaiser, R. Rebhi, S. Tanzilli","submitted_at":"2015-02-27T11:36:01Z","abstract_excerpt":"The complex internal atomic structure involved in radiative transitions has an effect on the spectrum of fluctuations (noise) of the transmitted light. A degenerate transition has different properties in this respect than a pure two-level transition. We investigate these variations by studying a certain transition between two degenerate atomic levels for different choices of the polarization state of the driving laser. For circular polarization, corresponding to the textbook two-level atom case, the optical spectrum shows the characteristic Mollow triplet for strong laser drive, while the corr"},"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":"1502.07868","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2015-02-27T11:36:01Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"927a50edc16716397415db42317fd7ef98ee3ee823399580a6b71616f94e04ad","abstract_canon_sha256":"742f145c730c2d4739844b7ed81feb739b253b337e5c79bbc025b22f211b965c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:29:03.081227Z","signature_b64":"9GOhVww213sWRDYiKbFpF/xxdQij83FIm1CKF2bguqT6pj/yKqufmXEUFhZ3p4eQWNT+PWNfOFYkuMhg4JEWCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0c470b6dc79aa42926ddc2a259649792134453998ccb1cd946f7f2167fdad79a","last_reissued_at":"2026-05-18T01:29:03.080483Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:29:03.080483Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fluctuation properties of laser light after interaction with an atomic system: comparison between two-level and multilevel atomic transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"A. Kastberg, A. Lezama, R. Kaiser, R. Rebhi, S. Tanzilli","submitted_at":"2015-02-27T11:36:01Z","abstract_excerpt":"The complex internal atomic structure involved in radiative transitions has an effect on the spectrum of fluctuations (noise) of the transmitted light. A degenerate transition has different properties in this respect than a pure two-level transition. We investigate these variations by studying a certain transition between two degenerate atomic levels for different choices of the polarization state of the driving laser. For circular polarization, corresponding to the textbook two-level atom case, the optical spectrum shows the characteristic Mollow triplet for strong laser drive, while the corr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.07868","kind":"arxiv","version":3},"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":"1502.07868","created_at":"2026-05-18T01:29:03.080567+00:00"},{"alias_kind":"arxiv_version","alias_value":"1502.07868v3","created_at":"2026-05-18T01:29:03.080567+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.07868","created_at":"2026-05-18T01:29:03.080567+00:00"},{"alias_kind":"pith_short_12","alias_value":"BRDQW3OHTKSC","created_at":"2026-05-18T12:29:14.074870+00:00"},{"alias_kind":"pith_short_16","alias_value":"BRDQW3OHTKSCSJW5","created_at":"2026-05-18T12:29:14.074870+00:00"},{"alias_kind":"pith_short_8","alias_value":"BRDQW3OH","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/BRDQW3OHTKSCSJW5YKRFSZEXSI","json":"https://pith.science/pith/BRDQW3OHTKSCSJW5YKRFSZEXSI.json","graph_json":"https://pith.science/api/pith-number/BRDQW3OHTKSCSJW5YKRFSZEXSI/graph.json","events_json":"https://pith.science/api/pith-number/BRDQW3OHTKSCSJW5YKRFSZEXSI/events.json","paper":"https://pith.science/paper/BRDQW3OH"},"agent_actions":{"view_html":"https://pith.science/pith/BRDQW3OHTKSCSJW5YKRFSZEXSI","download_json":"https://pith.science/pith/BRDQW3OHTKSCSJW5YKRFSZEXSI.json","view_paper":"https://pith.science/paper/BRDQW3OH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1502.07868&json=true","fetch_graph":"https://pith.science/api/pith-number/BRDQW3OHTKSCSJW5YKRFSZEXSI/graph.json","fetch_events":"https://pith.science/api/pith-number/BRDQW3OHTKSCSJW5YKRFSZEXSI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BRDQW3OHTKSCSJW5YKRFSZEXSI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BRDQW3OHTKSCSJW5YKRFSZEXSI/action/storage_attestation","attest_author":"https://pith.science/pith/BRDQW3OHTKSCSJW5YKRFSZEXSI/action/author_attestation","sign_citation":"https://pith.science/pith/BRDQW3OHTKSCSJW5YKRFSZEXSI/action/citation_signature","submit_replication":"https://pith.science/pith/BRDQW3OHTKSCSJW5YKRFSZEXSI/action/replication_record"}},"created_at":"2026-05-18T01:29:03.080567+00:00","updated_at":"2026-05-18T01:29:03.080567+00:00"}