{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:BJLTWDP645MQ5VIPQGZRSHG6E2","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":"b0cf1dd1135ae6a9e71a9b3f16966b37b477c477fb5eecea154eded980486f01","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-09-15T12:02:04Z","title_canon_sha256":"09d1a56e89dcec97d53f91b684c272ffb91f1387d29021d1c52e74a3d766ce50"},"schema_version":"1.0","source":{"id":"1209.3395","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1209.3395","created_at":"2026-05-18T03:16:06Z"},{"alias_kind":"arxiv_version","alias_value":"1209.3395v3","created_at":"2026-05-18T03:16:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1209.3395","created_at":"2026-05-18T03:16:06Z"},{"alias_kind":"pith_short_12","alias_value":"BJLTWDP645MQ","created_at":"2026-05-18T12:27:01Z"},{"alias_kind":"pith_short_16","alias_value":"BJLTWDP645MQ5VIP","created_at":"2026-05-18T12:27:01Z"},{"alias_kind":"pith_short_8","alias_value":"BJLTWDP6","created_at":"2026-05-18T12:27:01Z"}],"graph_snapshots":[{"event_id":"sha256:0d0e5552fdaa40b2924d2d89b5bffb3b6231339517a61a62ba9fb27403786438","target":"graph","created_at":"2026-05-18T03:16:06Z","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 the efficient free-space excitation of high-Q resonance modes in deformed microcavities via dynamical tunneling-assisted coupling. A quantum scattering theory is employed to study the free-space transmission properties, and it is found that the transmission includes the contribution from (1) the off-resonance background and (2) the on-resonance modulation, corresponding to the absence and presence of high-Q modes, respectively. The theory predicts asymmetric Fano-like resonances around high-Q modes in background transmission spectra, which are in good agreement with our recent e","authors_text":"Linbo Shao, Qi-Fan Yang, Xue-Feng Jiang, Ya-Long Cui, Yun-Feng Xiao","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-09-15T12:02:04Z","title":"Dynamical tunneling-assisted coupling of high-Q deformed microcavities using a free-space beam"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1209.3395","kind":"arxiv","version":3},"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":"sha256:91aa4a0bd204daf922ae395a245c7087a003baec03f8e832c4b32473f39f27c0","target":"record","created_at":"2026-05-18T03:16:06Z","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":"b0cf1dd1135ae6a9e71a9b3f16966b37b477c477fb5eecea154eded980486f01","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-09-15T12:02:04Z","title_canon_sha256":"09d1a56e89dcec97d53f91b684c272ffb91f1387d29021d1c52e74a3d766ce50"},"schema_version":"1.0","source":{"id":"1209.3395","kind":"arxiv","version":3}},"canonical_sha256":"0a573b0dfee7590ed50f81b3191cde269bcf04d6aceba5c6f15e24ed42f8c37d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0a573b0dfee7590ed50f81b3191cde269bcf04d6aceba5c6f15e24ed42f8c37d","first_computed_at":"2026-05-18T03:16:06.402849Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:16:06.402849Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4OdddmyqEs0vxMHgyaMKjcG85ePIwEB1/3spneaF2hl06Cd8IlGAADwDPYAh224w62f/IlZv5bJaUeHtXzQbBg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:16:06.403587Z","signed_message":"canonical_sha256_bytes"},"source_id":"1209.3395","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:91aa4a0bd204daf922ae395a245c7087a003baec03f8e832c4b32473f39f27c0","sha256:0d0e5552fdaa40b2924d2d89b5bffb3b6231339517a61a62ba9fb27403786438"],"state_sha256":"26f1ed5c13fa939af9276e71dd360587f4a279cd0fd3eb78c346a33cbbac8918"}