{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:YXJXJKZA45IPDWQGKIF2WEE435","short_pith_number":"pith:YXJXJKZA","canonical_record":{"source":{"id":"1202.5613","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-02-25T05:45:38Z","cross_cats_sorted":["physics.class-ph"],"title_canon_sha256":"0ac34e56fbe0e86d2ea1be51c7395db64ec649057fdff303aea877c92524a87d","abstract_canon_sha256":"bd0ab7addd3ce3571bf02ac0d2f38a0521d4754d3842e0c8298f1564d5cf7a9c"},"schema_version":"1.0"},"canonical_sha256":"c5d374ab20e750f1da06520bab109cdf4bb1bae438b5acf4a306ed36234f135c","source":{"kind":"arxiv","id":"1202.5613","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1202.5613","created_at":"2026-05-18T04:01:25Z"},{"alias_kind":"arxiv_version","alias_value":"1202.5613v1","created_at":"2026-05-18T04:01:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.5613","created_at":"2026-05-18T04:01:25Z"},{"alias_kind":"pith_short_12","alias_value":"YXJXJKZA45IP","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"YXJXJKZA45IPDWQG","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"YXJXJKZA","created_at":"2026-05-18T12:27:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:YXJXJKZA45IPDWQGKIF2WEE435","target":"record","payload":{"canonical_record":{"source":{"id":"1202.5613","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-02-25T05:45:38Z","cross_cats_sorted":["physics.class-ph"],"title_canon_sha256":"0ac34e56fbe0e86d2ea1be51c7395db64ec649057fdff303aea877c92524a87d","abstract_canon_sha256":"bd0ab7addd3ce3571bf02ac0d2f38a0521d4754d3842e0c8298f1564d5cf7a9c"},"schema_version":"1.0"},"canonical_sha256":"c5d374ab20e750f1da06520bab109cdf4bb1bae438b5acf4a306ed36234f135c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:01:25.278235Z","signature_b64":"l3nm0iWiZGCAlSW9dlK8y687bJ+vbFo6q980djRSAm2G3pAgr+ZIX+0dvplGs4IgRdwrdYkkGkRUeKRYyDldCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c5d374ab20e750f1da06520bab109cdf4bb1bae438b5acf4a306ed36234f135c","last_reissued_at":"2026-05-18T04:01:25.277594Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:01:25.277594Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1202.5613","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:01:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"a2HKuCe14BiJkzj4HX378etbHyPnSeFLlLYyuuSaTPnN+Oxu6rcsBSyUtPHbIVIbMiL1OgchG4QTHp1fXa1jDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T16:58:51.062085Z"},"content_sha256":"0ea2cc0f05e02767499acec461dfcb8357069d733bffa4af54c7fa5d090e7604","schema_version":"1.0","event_id":"sha256:0ea2cc0f05e02767499acec461dfcb8357069d733bffa4af54c7fa5d090e7604"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:YXJXJKZA45IPDWQGKIF2WEE435","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Anisotropy-induced Fano resonance","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.class-ph"],"primary_cat":"physics.optics","authors_text":"Andrey Novitsky, Boris Luk'yanchuk, Cheng-Wei Qiu, Jian-Wen Dong, Lei Gao","submitted_at":"2012-02-25T05:45:38Z","abstract_excerpt":"An optical Fano resonance, which is caused by birefringence control rather than frequency selection, is discovered. Such birefringence-induced Fano resonance comes with fast-switching radiation. The resonance condition $\\varepsilon_t< 1/\\varepsilon_r$ is revealed and a tiny perturbation in birefringence is found to result in a giant switch in the principal light pole induced near surface plasmon resonance. The loss and size effects upon the Fano resonance have been studied Fano resonance is still pronounced, even if the loss and size of the object increase. The evolutions of the radiation patt"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.5613","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:01:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AMkTb6TsFhyelBqFIMzLWlZF2ABHRSzKRrJYQzihgJxc340HB4LVrKIJzyLzhVS0k7QsmrHPC9mNnCEmkgIkCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T16:58:51.062451Z"},"content_sha256":"23932fa7a00ba46803c1557cafa84d1c9cd88c8f774f802542dd34233617c58c","schema_version":"1.0","event_id":"sha256:23932fa7a00ba46803c1557cafa84d1c9cd88c8f774f802542dd34233617c58c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YXJXJKZA45IPDWQGKIF2WEE435/bundle.json","state_url":"https://pith.science/pith/YXJXJKZA45IPDWQGKIF2WEE435/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YXJXJKZA45IPDWQGKIF2WEE435/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":"2026-06-01T16:58:51Z","links":{"resolver":"https://pith.science/pith/YXJXJKZA45IPDWQGKIF2WEE435","bundle":"https://pith.science/pith/YXJXJKZA45IPDWQGKIF2WEE435/bundle.json","state":"https://pith.science/pith/YXJXJKZA45IPDWQGKIF2WEE435/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YXJXJKZA45IPDWQGKIF2WEE435/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:YXJXJKZA45IPDWQGKIF2WEE435","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":"bd0ab7addd3ce3571bf02ac0d2f38a0521d4754d3842e0c8298f1564d5cf7a9c","cross_cats_sorted":["physics.class-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-02-25T05:45:38Z","title_canon_sha256":"0ac34e56fbe0e86d2ea1be51c7395db64ec649057fdff303aea877c92524a87d"},"schema_version":"1.0","source":{"id":"1202.5613","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1202.5613","created_at":"2026-05-18T04:01:25Z"},{"alias_kind":"arxiv_version","alias_value":"1202.5613v1","created_at":"2026-05-18T04:01:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.5613","created_at":"2026-05-18T04:01:25Z"},{"alias_kind":"pith_short_12","alias_value":"YXJXJKZA45IP","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"YXJXJKZA45IPDWQG","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"YXJXJKZA","created_at":"2026-05-18T12:27:30Z"}],"graph_snapshots":[{"event_id":"sha256:23932fa7a00ba46803c1557cafa84d1c9cd88c8f774f802542dd34233617c58c","target":"graph","created_at":"2026-05-18T04:01:25Z","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":"An optical Fano resonance, which is caused by birefringence control rather than frequency selection, is discovered. Such birefringence-induced Fano resonance comes with fast-switching radiation. The resonance condition $\\varepsilon_t< 1/\\varepsilon_r$ is revealed and a tiny perturbation in birefringence is found to result in a giant switch in the principal light pole induced near surface plasmon resonance. The loss and size effects upon the Fano resonance have been studied Fano resonance is still pronounced, even if the loss and size of the object increase. The evolutions of the radiation patt","authors_text":"Andrey Novitsky, Boris Luk'yanchuk, Cheng-Wei Qiu, Jian-Wen Dong, Lei Gao","cross_cats":["physics.class-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-02-25T05:45:38Z","title":"Anisotropy-induced Fano resonance"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.5613","kind":"arxiv","version":1},"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":"sha256:0ea2cc0f05e02767499acec461dfcb8357069d733bffa4af54c7fa5d090e7604","target":"record","created_at":"2026-05-18T04:01:25Z","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":"bd0ab7addd3ce3571bf02ac0d2f38a0521d4754d3842e0c8298f1564d5cf7a9c","cross_cats_sorted":["physics.class-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2012-02-25T05:45:38Z","title_canon_sha256":"0ac34e56fbe0e86d2ea1be51c7395db64ec649057fdff303aea877c92524a87d"},"schema_version":"1.0","source":{"id":"1202.5613","kind":"arxiv","version":1}},"canonical_sha256":"c5d374ab20e750f1da06520bab109cdf4bb1bae438b5acf4a306ed36234f135c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c5d374ab20e750f1da06520bab109cdf4bb1bae438b5acf4a306ed36234f135c","first_computed_at":"2026-05-18T04:01:25.277594Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:01:25.277594Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"l3nm0iWiZGCAlSW9dlK8y687bJ+vbFo6q980djRSAm2G3pAgr+ZIX+0dvplGs4IgRdwrdYkkGkRUeKRYyDldCg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:01:25.278235Z","signed_message":"canonical_sha256_bytes"},"source_id":"1202.5613","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0ea2cc0f05e02767499acec461dfcb8357069d733bffa4af54c7fa5d090e7604","sha256:23932fa7a00ba46803c1557cafa84d1c9cd88c8f774f802542dd34233617c58c"],"state_sha256":"5f68995f65ae718c110a5dec5e110a48f0fef316413abf724652b1d4cf1e2513"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AsW2vHztG0gDfMo9Ir13UAH3mcnxyx94d//smwCDn9HEpl1h/UKGJpGkcGiSXIzrlEQJVX+pjWrYG9+++tmqAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T16:58:51.064463Z","bundle_sha256":"109f9bb6d9a4bf8d1bbc63714039485cad243b94c48f636d7995b9aa91898c81"}}