{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:PI5BRGY2KA4UCDEP324NNA7TAK","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":"5ade661e89b7143701ac67f13c25320165a7ff942b7651b4a60954aef448f0b9","cross_cats_sorted":["cond-mat.mes-hall","physics.atom-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-09-02T20:58:29Z","title_canon_sha256":"b3004fa2f260857412ad2f1b79719f2353700af8732284c8444941590abbb0dc"},"schema_version":"1.0","source":{"id":"1309.0538","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1309.0538","created_at":"2026-05-18T01:47:50Z"},{"alias_kind":"arxiv_version","alias_value":"1309.0538v2","created_at":"2026-05-18T01:47:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1309.0538","created_at":"2026-05-18T01:47:50Z"},{"alias_kind":"pith_short_12","alias_value":"PI5BRGY2KA4U","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_16","alias_value":"PI5BRGY2KA4UCDEP","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_8","alias_value":"PI5BRGY2","created_at":"2026-05-18T12:27:54Z"}],"graph_snapshots":[{"event_id":"sha256:4ffe00e4953ab9ca33e9ee29b1cecfd1dac746427f41a924e684577f9c87247e","target":"graph","created_at":"2026-05-18T01:47:50Z","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":"We investigate optical bistability in a multilayer one-dimensional photonic crystal where the central layer is doped with $\\Lambda$-type three level atoms. We take into account the influence of spontaneously generated coherence when the lower atomic levels are sufficiently close to each other, in which case Kerr-type nonlinear response of the atoms is enhanced. We calculate the propagation of a probe beam in the defect mode window using numerical nonlinear transfer matrix method. We find that Rabi frequency of a control field acting on the defect layer and the detuning of the probe field from ","authors_text":"\\\"Ozg\\\"ur E. M\\\"ustecaplio\\u{g}lu, Shahnaz Aas","cross_cats":["cond-mat.mes-hall","physics.atom-ph","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-09-02T20:58:29Z","title":"Optical bistability in one dimensional doped photonic crystals with spontaneously generated coherence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1309.0538","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:e3e27f02487e9184377b8fb7f3a70d530578e90a0b8e964dc254cfea74ef8f2f","target":"record","created_at":"2026-05-18T01:47:50Z","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":"5ade661e89b7143701ac67f13c25320165a7ff942b7651b4a60954aef448f0b9","cross_cats_sorted":["cond-mat.mes-hall","physics.atom-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-09-02T20:58:29Z","title_canon_sha256":"b3004fa2f260857412ad2f1b79719f2353700af8732284c8444941590abbb0dc"},"schema_version":"1.0","source":{"id":"1309.0538","kind":"arxiv","version":2}},"canonical_sha256":"7a3a189b1a5039410c8fdeb8d683f302aca0ac09bb27f78aba7304cc6beb2a3d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7a3a189b1a5039410c8fdeb8d683f302aca0ac09bb27f78aba7304cc6beb2a3d","first_computed_at":"2026-05-18T01:47:50.534764Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:47:50.534764Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"SJoJicUic4TK+zbT3FNPvUsMhx5qVR0VaoKty5kttrR+pjfZNm32KsP1stYDsqhxB6gk5a41zKw80c4gFThHCg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:47:50.535130Z","signed_message":"canonical_sha256_bytes"},"source_id":"1309.0538","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e3e27f02487e9184377b8fb7f3a70d530578e90a0b8e964dc254cfea74ef8f2f","sha256:4ffe00e4953ab9ca33e9ee29b1cecfd1dac746427f41a924e684577f9c87247e"],"state_sha256":"7d36c326513ee93a0c93bdafa9b4051b85c89a780997309d4c5a657df3d92a49"}