{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:AYNJXFY2NPQMJX77EJCMUC5O55","short_pith_number":"pith:AYNJXFY2","schema_version":"1.0","canonical_sha256":"061a9b971a6be0c4dfff2244ca0baeef7af333a92b334f1d67a30fff7a14869d","source":{"kind":"arxiv","id":"1409.3598","version":1},"attestation_state":"computed","paper":{"title":"Electromagnetically induced transparency with Laguerre-Gaussian modes in ultracold rubidium","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"A. M. Marino, E. R. I. Abraham, S. P. Krzyzewski, T. G. Akin","submitted_at":"2014-09-11T21:15:36Z","abstract_excerpt":"We demonstrate electromagnetically induced transparency with the control laser in a Laguerre-Gaussian mode. The transmission spectrum is studied in an ultracold gas for the D2 line in both $^{85}$Rb and $^{87}$Rb, where the decoherence due to diffusion of the atomic medium is negligible. We compare these results to a similar configuration, but with the control laser in the fundamental laser mode. We model the transmission of a probe laser under both configurations, and we find good agreement with the experiment. We conclude that the use of Laguerre-Gaussian modes in electromagnetically induced"},"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":"1409.3598","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-09-11T21:15:36Z","cross_cats_sorted":[],"title_canon_sha256":"fc7fb8b13c168eaf9a0158ba1fa464bfe58cad01e509da778e7179fd94c85e06","abstract_canon_sha256":"4854e4126a0baeddae48582db9c787c2dfe1068ed0b185c5996e7949928eb84d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:43:00.170526Z","signature_b64":"1eiwE8AOBGRGs/xgPwnaXp4ZofE9jmsRuYW3RWP5SC3FoVpf2m1Gr9HtJtOi4bwH5V5my+6uNJjIMoNPPzKQCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"061a9b971a6be0c4dfff2244ca0baeef7af333a92b334f1d67a30fff7a14869d","last_reissued_at":"2026-05-18T02:43:00.169995Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:43:00.169995Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electromagnetically induced transparency with Laguerre-Gaussian modes in ultracold rubidium","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"A. M. Marino, E. R. I. Abraham, S. P. Krzyzewski, T. G. Akin","submitted_at":"2014-09-11T21:15:36Z","abstract_excerpt":"We demonstrate electromagnetically induced transparency with the control laser in a Laguerre-Gaussian mode. The transmission spectrum is studied in an ultracold gas for the D2 line in both $^{85}$Rb and $^{87}$Rb, where the decoherence due to diffusion of the atomic medium is negligible. We compare these results to a similar configuration, but with the control laser in the fundamental laser mode. We model the transmission of a probe laser under both configurations, and we find good agreement with the experiment. We conclude that the use of Laguerre-Gaussian modes in electromagnetically induced"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.3598","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":"1409.3598","created_at":"2026-05-18T02:43:00.170082+00:00"},{"alias_kind":"arxiv_version","alias_value":"1409.3598v1","created_at":"2026-05-18T02:43:00.170082+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.3598","created_at":"2026-05-18T02:43:00.170082+00:00"},{"alias_kind":"pith_short_12","alias_value":"AYNJXFY2NPQM","created_at":"2026-05-18T12:28:19.803747+00:00"},{"alias_kind":"pith_short_16","alias_value":"AYNJXFY2NPQMJX77","created_at":"2026-05-18T12:28:19.803747+00:00"},{"alias_kind":"pith_short_8","alias_value":"AYNJXFY2","created_at":"2026-05-18T12:28:19.803747+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/AYNJXFY2NPQMJX77EJCMUC5O55","json":"https://pith.science/pith/AYNJXFY2NPQMJX77EJCMUC5O55.json","graph_json":"https://pith.science/api/pith-number/AYNJXFY2NPQMJX77EJCMUC5O55/graph.json","events_json":"https://pith.science/api/pith-number/AYNJXFY2NPQMJX77EJCMUC5O55/events.json","paper":"https://pith.science/paper/AYNJXFY2"},"agent_actions":{"view_html":"https://pith.science/pith/AYNJXFY2NPQMJX77EJCMUC5O55","download_json":"https://pith.science/pith/AYNJXFY2NPQMJX77EJCMUC5O55.json","view_paper":"https://pith.science/paper/AYNJXFY2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1409.3598&json=true","fetch_graph":"https://pith.science/api/pith-number/AYNJXFY2NPQMJX77EJCMUC5O55/graph.json","fetch_events":"https://pith.science/api/pith-number/AYNJXFY2NPQMJX77EJCMUC5O55/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AYNJXFY2NPQMJX77EJCMUC5O55/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AYNJXFY2NPQMJX77EJCMUC5O55/action/storage_attestation","attest_author":"https://pith.science/pith/AYNJXFY2NPQMJX77EJCMUC5O55/action/author_attestation","sign_citation":"https://pith.science/pith/AYNJXFY2NPQMJX77EJCMUC5O55/action/citation_signature","submit_replication":"https://pith.science/pith/AYNJXFY2NPQMJX77EJCMUC5O55/action/replication_record"}},"created_at":"2026-05-18T02:43:00.170082+00:00","updated_at":"2026-05-18T02:43:00.170082+00:00"}