{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:6ZBSTH27XAQAQKBQM54PKPNULX","short_pith_number":"pith:6ZBSTH27","canonical_record":{"source":{"id":"1606.09411","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-06-30T09:46:06Z","cross_cats_sorted":[],"title_canon_sha256":"a94101198611021289a621bdf59580ddbf8042a1cb1a649c6d02d1a90fb2b7f7","abstract_canon_sha256":"fb0582c8d31ce569ea48b17d1be55df87fe98afa4098378bca9ed2dec6d739a0"},"schema_version":"1.0"},"canonical_sha256":"f643299f5fb8200828306778f53db45dedd1f491219efb0f4e5e283b20fb9b75","source":{"kind":"arxiv","id":"1606.09411","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.09411","created_at":"2026-05-18T01:00:12Z"},{"alias_kind":"arxiv_version","alias_value":"1606.09411v2","created_at":"2026-05-18T01:00:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.09411","created_at":"2026-05-18T01:00:12Z"},{"alias_kind":"pith_short_12","alias_value":"6ZBSTH27XAQA","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"6ZBSTH27XAQAQKBQ","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"6ZBSTH27","created_at":"2026-05-18T12:30:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:6ZBSTH27XAQAQKBQM54PKPNULX","target":"record","payload":{"canonical_record":{"source":{"id":"1606.09411","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-06-30T09:46:06Z","cross_cats_sorted":[],"title_canon_sha256":"a94101198611021289a621bdf59580ddbf8042a1cb1a649c6d02d1a90fb2b7f7","abstract_canon_sha256":"fb0582c8d31ce569ea48b17d1be55df87fe98afa4098378bca9ed2dec6d739a0"},"schema_version":"1.0"},"canonical_sha256":"f643299f5fb8200828306778f53db45dedd1f491219efb0f4e5e283b20fb9b75","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:00:12.236799Z","signature_b64":"jrduINgwZ9X7hWARMZuAQjs8U3envd+sHQZcRdWowmTy0a4t/jW+3gPHvK4PblfHH5F4Pq2SUfuN7NJ8su77Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f643299f5fb8200828306778f53db45dedd1f491219efb0f4e5e283b20fb9b75","last_reissued_at":"2026-05-18T01:00:12.236215Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:00:12.236215Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1606.09411","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:00:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gpUG5+2Kia44yZ+mRq34Xnh5m0TeHk6av7cemfLaiTj9gj2j0EEljBdqEcJ7c1v6HRZvR6AwWk0y/tVj0Iy2AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T06:54:34.202538Z"},"content_sha256":"345870e86f0f8c8b4aff87d0454a4a996a523862e7429f0cc2e99d556580204d","schema_version":"1.0","event_id":"sha256:345870e86f0f8c8b4aff87d0454a4a996a523862e7429f0cc2e99d556580204d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:6ZBSTH27XAQAQKBQM54PKPNULX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Role of dressed-state interference in electromagnetically induced transparency","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Sumanta Khan, Vasant Natarajan, Vineet Bharti","submitted_at":"2016-06-30T09:46:06Z","abstract_excerpt":"Electromagnetically induced transparency (EIT) in three-level systems uses a strong control laser on one transition to modify the absorption of a weak probe laser on a second transition. The control laser creates dressed states whose decay pathways show interference. We study the role of dressed-state interference in causing EIT in the three types of three-level systems -- lambda ($\\Lambda$), ladder ($\\Xi$), and vee (V). In order to get realistic values for the linewidths of the energy levels involved, we consider appropriate hyperfine levels of $^{87}$Rb. For such realistic systems, we find t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.09411","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":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:00:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zWpUfkhlqTedk2kn/P+4e7UkWMuSdvmKY88f+V2erloptDnYkCECbO0xWHkeY3Rw1Kn+qI0ok/pY8yweyTVFCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T06:54:34.202894Z"},"content_sha256":"5a202a6b068b54e033b2a04eaa7d30a91b88da1f78b02cef478c1db8efe740bd","schema_version":"1.0","event_id":"sha256:5a202a6b068b54e033b2a04eaa7d30a91b88da1f78b02cef478c1db8efe740bd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6ZBSTH27XAQAQKBQM54PKPNULX/bundle.json","state_url":"https://pith.science/pith/6ZBSTH27XAQAQKBQM54PKPNULX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6ZBSTH27XAQAQKBQM54PKPNULX/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-03T06:54:34Z","links":{"resolver":"https://pith.science/pith/6ZBSTH27XAQAQKBQM54PKPNULX","bundle":"https://pith.science/pith/6ZBSTH27XAQAQKBQM54PKPNULX/bundle.json","state":"https://pith.science/pith/6ZBSTH27XAQAQKBQM54PKPNULX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6ZBSTH27XAQAQKBQM54PKPNULX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:6ZBSTH27XAQAQKBQM54PKPNULX","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"fb0582c8d31ce569ea48b17d1be55df87fe98afa4098378bca9ed2dec6d739a0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-06-30T09:46:06Z","title_canon_sha256":"a94101198611021289a621bdf59580ddbf8042a1cb1a649c6d02d1a90fb2b7f7"},"schema_version":"1.0","source":{"id":"1606.09411","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.09411","created_at":"2026-05-18T01:00:12Z"},{"alias_kind":"arxiv_version","alias_value":"1606.09411v2","created_at":"2026-05-18T01:00:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.09411","created_at":"2026-05-18T01:00:12Z"},{"alias_kind":"pith_short_12","alias_value":"6ZBSTH27XAQA","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"6ZBSTH27XAQAQKBQ","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"6ZBSTH27","created_at":"2026-05-18T12:30:04Z"}],"graph_snapshots":[{"event_id":"sha256:5a202a6b068b54e033b2a04eaa7d30a91b88da1f78b02cef478c1db8efe740bd","target":"graph","created_at":"2026-05-18T01:00:12Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Electromagnetically induced transparency (EIT) in three-level systems uses a strong control laser on one transition to modify the absorption of a weak probe laser on a second transition. The control laser creates dressed states whose decay pathways show interference. We study the role of dressed-state interference in causing EIT in the three types of three-level systems -- lambda ($\\Lambda$), ladder ($\\Xi$), and vee (V). In order to get realistic values for the linewidths of the energy levels involved, we consider appropriate hyperfine levels of $^{87}$Rb. For such realistic systems, we find t","authors_text":"Sumanta Khan, Vasant Natarajan, Vineet Bharti","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-06-30T09:46:06Z","title":"Role of dressed-state interference in electromagnetically induced transparency"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.09411","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:345870e86f0f8c8b4aff87d0454a4a996a523862e7429f0cc2e99d556580204d","target":"record","created_at":"2026-05-18T01:00:12Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"fb0582c8d31ce569ea48b17d1be55df87fe98afa4098378bca9ed2dec6d739a0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-06-30T09:46:06Z","title_canon_sha256":"a94101198611021289a621bdf59580ddbf8042a1cb1a649c6d02d1a90fb2b7f7"},"schema_version":"1.0","source":{"id":"1606.09411","kind":"arxiv","version":2}},"canonical_sha256":"f643299f5fb8200828306778f53db45dedd1f491219efb0f4e5e283b20fb9b75","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f643299f5fb8200828306778f53db45dedd1f491219efb0f4e5e283b20fb9b75","first_computed_at":"2026-05-18T01:00:12.236215Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:00:12.236215Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jrduINgwZ9X7hWARMZuAQjs8U3envd+sHQZcRdWowmTy0a4t/jW+3gPHvK4PblfHH5F4Pq2SUfuN7NJ8su77Dg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:00:12.236799Z","signed_message":"canonical_sha256_bytes"},"source_id":"1606.09411","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:345870e86f0f8c8b4aff87d0454a4a996a523862e7429f0cc2e99d556580204d","sha256:5a202a6b068b54e033b2a04eaa7d30a91b88da1f78b02cef478c1db8efe740bd"],"state_sha256":"a3ace360860268c429c6a435802531b8483e9c569b6b78c5f8002449e575f575"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JW1Ike37FHFxLmfKAJgBYRC630EdAvzUAifkIW00GUNJYkw/hs0hPKcI9pePRdwQ7bbl8Qxrju22+OTF/simAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T06:54:34.204951Z","bundle_sha256":"0386592cff2d044ef358b5d4bd49f9e762444b164b38dc5a9b3006dfdf5111ae"}}