{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:TAW74EXR32IBGUQIUG7TPUCTEU","short_pith_number":"pith:TAW74EXR","schema_version":"1.0","canonical_sha256":"982dfe12f1de90135208a1bf37d053252842ea98b3a713cb2d2ecda773e3ac85","source":{"kind":"arxiv","id":"2412.15038","version":3},"attestation_state":"computed","paper":{"title":"Emergence of a Landau level structure in dark optical lattices","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Jean Dalibard, Sylvain Nascimbene","submitted_at":"2024-12-19T16:50:22Z","abstract_excerpt":"An optical flux lattice is a set of light beams that couple different internal states of an atom, thereby producing topological energy bands. Here we present a configuration in which the atoms exhibit a dark state, i.e. an internal state that is not coupled to the light. At large light intensity, the low-energy dynamics is restricted to the dark state, leading to an effective continuum model with a Landau-level-like structure. This structure is dramatically different from that of usual topological optical lattices, which lead to discrete models in the tight-binding limit. For well-chosen atomi"},"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":"2412.15038","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2024-12-19T16:50:22Z","cross_cats_sorted":[],"title_canon_sha256":"1eaef4b923ea0dbc5971ec83190e66075eee9efed218c0e84f7b229302800a7c","abstract_canon_sha256":"3bf4dbacb85d1bf4e2d353188cc657a7c6303afc2bfc3c58e9842e5956339cee"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T12:04:13.561638Z","signature_b64":"a8qp0YG9vrX2a74Z+J+U6iaoNIjFs69VtA4AsbLVWQD/2sKB03U+r9Ly3+aiMJkxCcZ+0fRmo05jp0seIf60DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"982dfe12f1de90135208a1bf37d053252842ea98b3a713cb2d2ecda773e3ac85","last_reissued_at":"2026-07-05T12:04:13.561107Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T12:04:13.561107Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Emergence of a Landau level structure in dark optical lattices","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.quant-gas","authors_text":"Jean Dalibard, Sylvain Nascimbene","submitted_at":"2024-12-19T16:50:22Z","abstract_excerpt":"An optical flux lattice is a set of light beams that couple different internal states of an atom, thereby producing topological energy bands. Here we present a configuration in which the atoms exhibit a dark state, i.e. an internal state that is not coupled to the light. At large light intensity, the low-energy dynamics is restricted to the dark state, leading to an effective continuum model with a Landau-level-like structure. This structure is dramatically different from that of usual topological optical lattices, which lead to discrete models in the tight-binding limit. For well-chosen atomi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.15038","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2412.15038/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2412.15038","created_at":"2026-07-05T12:04:13.561172+00:00"},{"alias_kind":"arxiv_version","alias_value":"2412.15038v3","created_at":"2026-07-05T12:04:13.561172+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.15038","created_at":"2026-07-05T12:04:13.561172+00:00"},{"alias_kind":"pith_short_12","alias_value":"TAW74EXR32IB","created_at":"2026-07-05T12:04:13.561172+00:00"},{"alias_kind":"pith_short_16","alias_value":"TAW74EXR32IBGUQI","created_at":"2026-07-05T12:04:13.561172+00:00"},{"alias_kind":"pith_short_8","alias_value":"TAW74EXR","created_at":"2026-07-05T12:04:13.561172+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.01481","citing_title":"Ideal Optical Flux Lattices","ref_index":47,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TAW74EXR32IBGUQIUG7TPUCTEU","json":"https://pith.science/pith/TAW74EXR32IBGUQIUG7TPUCTEU.json","graph_json":"https://pith.science/api/pith-number/TAW74EXR32IBGUQIUG7TPUCTEU/graph.json","events_json":"https://pith.science/api/pith-number/TAW74EXR32IBGUQIUG7TPUCTEU/events.json","paper":"https://pith.science/paper/TAW74EXR"},"agent_actions":{"view_html":"https://pith.science/pith/TAW74EXR32IBGUQIUG7TPUCTEU","download_json":"https://pith.science/pith/TAW74EXR32IBGUQIUG7TPUCTEU.json","view_paper":"https://pith.science/paper/TAW74EXR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2412.15038&json=true","fetch_graph":"https://pith.science/api/pith-number/TAW74EXR32IBGUQIUG7TPUCTEU/graph.json","fetch_events":"https://pith.science/api/pith-number/TAW74EXR32IBGUQIUG7TPUCTEU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TAW74EXR32IBGUQIUG7TPUCTEU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TAW74EXR32IBGUQIUG7TPUCTEU/action/storage_attestation","attest_author":"https://pith.science/pith/TAW74EXR32IBGUQIUG7TPUCTEU/action/author_attestation","sign_citation":"https://pith.science/pith/TAW74EXR32IBGUQIUG7TPUCTEU/action/citation_signature","submit_replication":"https://pith.science/pith/TAW74EXR32IBGUQIUG7TPUCTEU/action/replication_record"}},"created_at":"2026-07-05T12:04:13.561172+00:00","updated_at":"2026-07-05T12:04:13.561172+00:00"}