{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:UL4RUFH7HI6LORDHZKCCVR243K","short_pith_number":"pith:UL4RUFH7","schema_version":"1.0","canonical_sha256":"a2f91a14ff3a3cb74467ca842ac75cdaa9dd2321842f09b904b46ac21f7f6cf8","source":{"kind":"arxiv","id":"2412.02541","version":2},"attestation_state":"computed","paper":{"title":"Single-atom resolved collective spectroscopy of a one-dimensional atomic array","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"Antoine Browaeys, Britton Hofer, Damien Bloch, Giulio Biagioni, Igor Ferrier-Barbut, Nathan Bonvalet","submitted_at":"2024-12-03T16:34:32Z","abstract_excerpt":"Ordered atomic arrays feature an enhanced collective optical response compared to random atomic ensembles due to constructive interference in resonant dipole-dipole interactions. One consequence is the existence of a large shift of the transition with respect to the bare atomic frequency. In the linear optics regime (low light intensity), one observes a spectroscopic shift of the Lorentzian atomic line often called the collective Lamb shift. For stronger driving, many excitations are present in the system rendering the calculation of this shift theoretically challenging, but its understanding "},"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":"2412.02541","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2024-12-03T16:34:32Z","cross_cats_sorted":["cond-mat.quant-gas","physics.atom-ph"],"title_canon_sha256":"16631b1ae5c4990814c0d05935cc1be92cb30cd9116cfc487e405b41e855eaaf","abstract_canon_sha256":"a0b23827eceee8c042982b7a1b306dd385493eacb3876cb567ad6156f4c9811c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:41:36.913197Z","signature_b64":"Qal3OjrYKLpwTyMjZ2PdcOyf/rBI5G/a7VvErFJusWec1n0DT4lu0V39JdWbdE1FRyUKe5xMyEOalIc9/ev7DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a2f91a14ff3a3cb74467ca842ac75cdaa9dd2321842f09b904b46ac21f7f6cf8","last_reissued_at":"2026-07-05T11:41:36.912724Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:41:36.912724Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Single-atom resolved collective spectroscopy of a one-dimensional atomic array","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"Antoine Browaeys, Britton Hofer, Damien Bloch, Giulio Biagioni, Igor Ferrier-Barbut, Nathan Bonvalet","submitted_at":"2024-12-03T16:34:32Z","abstract_excerpt":"Ordered atomic arrays feature an enhanced collective optical response compared to random atomic ensembles due to constructive interference in resonant dipole-dipole interactions. One consequence is the existence of a large shift of the transition with respect to the bare atomic frequency. In the linear optics regime (low light intensity), one observes a spectroscopic shift of the Lorentzian atomic line often called the collective Lamb shift. For stronger driving, many excitations are present in the system rendering the calculation of this shift theoretically challenging, but its understanding "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.02541","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2412.02541/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":"2412.02541","created_at":"2026-07-05T11:41:36.912784+00:00"},{"alias_kind":"arxiv_version","alias_value":"2412.02541v2","created_at":"2026-07-05T11:41:36.912784+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.02541","created_at":"2026-07-05T11:41:36.912784+00:00"},{"alias_kind":"pith_short_12","alias_value":"UL4RUFH7HI6L","created_at":"2026-07-05T11:41:36.912784+00:00"},{"alias_kind":"pith_short_16","alias_value":"UL4RUFH7HI6LORDH","created_at":"2026-07-05T11:41:36.912784+00:00"},{"alias_kind":"pith_short_8","alias_value":"UL4RUFH7","created_at":"2026-07-05T11:41:36.912784+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.16549","citing_title":"Probing subradiant dynamics in cold atomic ensembles via population and emitted light measurements","ref_index":66,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UL4RUFH7HI6LORDHZKCCVR243K","json":"https://pith.science/pith/UL4RUFH7HI6LORDHZKCCVR243K.json","graph_json":"https://pith.science/api/pith-number/UL4RUFH7HI6LORDHZKCCVR243K/graph.json","events_json":"https://pith.science/api/pith-number/UL4RUFH7HI6LORDHZKCCVR243K/events.json","paper":"https://pith.science/paper/UL4RUFH7"},"agent_actions":{"view_html":"https://pith.science/pith/UL4RUFH7HI6LORDHZKCCVR243K","download_json":"https://pith.science/pith/UL4RUFH7HI6LORDHZKCCVR243K.json","view_paper":"https://pith.science/paper/UL4RUFH7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2412.02541&json=true","fetch_graph":"https://pith.science/api/pith-number/UL4RUFH7HI6LORDHZKCCVR243K/graph.json","fetch_events":"https://pith.science/api/pith-number/UL4RUFH7HI6LORDHZKCCVR243K/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UL4RUFH7HI6LORDHZKCCVR243K/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UL4RUFH7HI6LORDHZKCCVR243K/action/storage_attestation","attest_author":"https://pith.science/pith/UL4RUFH7HI6LORDHZKCCVR243K/action/author_attestation","sign_citation":"https://pith.science/pith/UL4RUFH7HI6LORDHZKCCVR243K/action/citation_signature","submit_replication":"https://pith.science/pith/UL4RUFH7HI6LORDHZKCCVR243K/action/replication_record"}},"created_at":"2026-07-05T11:41:36.912784+00:00","updated_at":"2026-07-05T11:41:36.912784+00:00"}