{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:I2BKDGFQEWYQIZS5EZ36FWXTZV","short_pith_number":"pith:I2BKDGFQ","canonical_record":{"source":{"id":"1404.7532","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-04-29T20:57:03Z","cross_cats_sorted":[],"title_canon_sha256":"346b33e7dfb50b562c87c4e26f843fde590dc3ef1ec0dec3e4f9e09caf2b41b3","abstract_canon_sha256":"694470291a7b50a24251197e4505cab7f58735ca128af5694e9af1291f3395bb"},"schema_version":"1.0"},"canonical_sha256":"4682a198b025b104665d2677e2daf3cd63a7c8016c54f162519598ed528eb38d","source":{"kind":"arxiv","id":"1404.7532","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.7532","created_at":"2026-05-18T01:43:21Z"},{"alias_kind":"arxiv_version","alias_value":"1404.7532v1","created_at":"2026-05-18T01:43:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.7532","created_at":"2026-05-18T01:43:21Z"},{"alias_kind":"pith_short_12","alias_value":"I2BKDGFQEWYQ","created_at":"2026-05-18T12:28:33Z"},{"alias_kind":"pith_short_16","alias_value":"I2BKDGFQEWYQIZS5","created_at":"2026-05-18T12:28:33Z"},{"alias_kind":"pith_short_8","alias_value":"I2BKDGFQ","created_at":"2026-05-18T12:28:33Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:I2BKDGFQEWYQIZS5EZ36FWXTZV","target":"record","payload":{"canonical_record":{"source":{"id":"1404.7532","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-04-29T20:57:03Z","cross_cats_sorted":[],"title_canon_sha256":"346b33e7dfb50b562c87c4e26f843fde590dc3ef1ec0dec3e4f9e09caf2b41b3","abstract_canon_sha256":"694470291a7b50a24251197e4505cab7f58735ca128af5694e9af1291f3395bb"},"schema_version":"1.0"},"canonical_sha256":"4682a198b025b104665d2677e2daf3cd63a7c8016c54f162519598ed528eb38d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:43:21.658308Z","signature_b64":"aIlf0j7W33un8Pf4UzKJAc5OZSnsJ5E6lg9tSa3+FB4Q63rZ6Bmrjl6QZFJLM7xlozauYhitYhLezp1YVj7BAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4682a198b025b104665d2677e2daf3cd63a7c8016c54f162519598ed528eb38d","last_reissued_at":"2026-05-18T01:43:21.657643Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:43:21.657643Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1404.7532","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":"2026-05-18T01:43:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zEMDFa7wU0XPK2cO4OeC/a2M3lz6M9U4/N01PEDjdefDdka4TrwzphJORQEH3M4sqzVZR1HaH3hYVB/nyW2LCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T15:29:46.405778Z"},"content_sha256":"e914929032dc556f1faeaa238a656dee4191f77d0ced39d49473a8dd227b9e9a","schema_version":"1.0","event_id":"sha256:e914929032dc556f1faeaa238a656dee4191f77d0ced39d49473a8dd227b9e9a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:I2BKDGFQEWYQIZS5EZ36FWXTZV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fano resonance control in a photonic crystal structure and its application to ultrafast switching","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Christophe Peucheret, Hao Hu, Jesper M{\\o}rk, Kresten Yvind, Leif Katsuo Oxenl{\\o}we, Mikkel Heuck, Weiqi Xue, Yaohui Chen, Yi Yu","submitted_at":"2014-04-29T20:57:03Z","abstract_excerpt":"Fano resonances appear in quantum mechanical as well as classical systems as a result of the interference between two paths: one involving a discrete resonance and the other a continuum. Compared to a conventional resonance, characterized by a Lorentzian spectral response, the characteristic asymmetric and sharp spectral response of a Fano resonance is suggested to enable photonic switches and sensors with superior characteristics. While experimental demonstrations of the appearance of Fano resonances have been made in both plasmonic and photonic-crystal structures, the control of these resona"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.7532","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":"2026-05-18T01:43:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0CcbHc0qW9FmfGeARkX7fltzAMhoNY+OEdMl8ZyXvHAxqLEZ8QGWQ+Qh4TwzR+0woHWQiotXxbzqQHbdh6RNCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T15:29:46.406505Z"},"content_sha256":"17917339c6d0ea73347a95f590a3a18ac99d40f34508223f7905ce13de0b219a","schema_version":"1.0","event_id":"sha256:17917339c6d0ea73347a95f590a3a18ac99d40f34508223f7905ce13de0b219a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/I2BKDGFQEWYQIZS5EZ36FWXTZV/bundle.json","state_url":"https://pith.science/pith/I2BKDGFQEWYQIZS5EZ36FWXTZV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/I2BKDGFQEWYQIZS5EZ36FWXTZV/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":"2026-05-27T15:29:46Z","links":{"resolver":"https://pith.science/pith/I2BKDGFQEWYQIZS5EZ36FWXTZV","bundle":"https://pith.science/pith/I2BKDGFQEWYQIZS5EZ36FWXTZV/bundle.json","state":"https://pith.science/pith/I2BKDGFQEWYQIZS5EZ36FWXTZV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/I2BKDGFQEWYQIZS5EZ36FWXTZV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:I2BKDGFQEWYQIZS5EZ36FWXTZV","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":"694470291a7b50a24251197e4505cab7f58735ca128af5694e9af1291f3395bb","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-04-29T20:57:03Z","title_canon_sha256":"346b33e7dfb50b562c87c4e26f843fde590dc3ef1ec0dec3e4f9e09caf2b41b3"},"schema_version":"1.0","source":{"id":"1404.7532","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.7532","created_at":"2026-05-18T01:43:21Z"},{"alias_kind":"arxiv_version","alias_value":"1404.7532v1","created_at":"2026-05-18T01:43:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.7532","created_at":"2026-05-18T01:43:21Z"},{"alias_kind":"pith_short_12","alias_value":"I2BKDGFQEWYQ","created_at":"2026-05-18T12:28:33Z"},{"alias_kind":"pith_short_16","alias_value":"I2BKDGFQEWYQIZS5","created_at":"2026-05-18T12:28:33Z"},{"alias_kind":"pith_short_8","alias_value":"I2BKDGFQ","created_at":"2026-05-18T12:28:33Z"}],"graph_snapshots":[{"event_id":"sha256:17917339c6d0ea73347a95f590a3a18ac99d40f34508223f7905ce13de0b219a","target":"graph","created_at":"2026-05-18T01:43:21Z","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":"Fano resonances appear in quantum mechanical as well as classical systems as a result of the interference between two paths: one involving a discrete resonance and the other a continuum. Compared to a conventional resonance, characterized by a Lorentzian spectral response, the characteristic asymmetric and sharp spectral response of a Fano resonance is suggested to enable photonic switches and sensors with superior characteristics. While experimental demonstrations of the appearance of Fano resonances have been made in both plasmonic and photonic-crystal structures, the control of these resona","authors_text":"Christophe Peucheret, Hao Hu, Jesper M{\\o}rk, Kresten Yvind, Leif Katsuo Oxenl{\\o}we, Mikkel Heuck, Weiqi Xue, Yaohui Chen, Yi Yu","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-04-29T20:57:03Z","title":"Fano resonance control in a photonic crystal structure and its application to ultrafast switching"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.7532","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:e914929032dc556f1faeaa238a656dee4191f77d0ced39d49473a8dd227b9e9a","target":"record","created_at":"2026-05-18T01:43:21Z","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":"694470291a7b50a24251197e4505cab7f58735ca128af5694e9af1291f3395bb","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-04-29T20:57:03Z","title_canon_sha256":"346b33e7dfb50b562c87c4e26f843fde590dc3ef1ec0dec3e4f9e09caf2b41b3"},"schema_version":"1.0","source":{"id":"1404.7532","kind":"arxiv","version":1}},"canonical_sha256":"4682a198b025b104665d2677e2daf3cd63a7c8016c54f162519598ed528eb38d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4682a198b025b104665d2677e2daf3cd63a7c8016c54f162519598ed528eb38d","first_computed_at":"2026-05-18T01:43:21.657643Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:43:21.657643Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"aIlf0j7W33un8Pf4UzKJAc5OZSnsJ5E6lg9tSa3+FB4Q63rZ6Bmrjl6QZFJLM7xlozauYhitYhLezp1YVj7BAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:43:21.658308Z","signed_message":"canonical_sha256_bytes"},"source_id":"1404.7532","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e914929032dc556f1faeaa238a656dee4191f77d0ced39d49473a8dd227b9e9a","sha256:17917339c6d0ea73347a95f590a3a18ac99d40f34508223f7905ce13de0b219a"],"state_sha256":"ef4561f776b571cf24913e94e7efd13f6119fe2db098fe20bca69b8a94e0c86a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PETmgqlYimtEmzG9SRxF6GygibpaJ7r6aNaOUqTUgXOE7vcCbbRAA6g3O1kEPD0fKqOmLtkDnyfqTsX369WSBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T15:29:46.410333Z","bundle_sha256":"a1abad4e0f5ff5df4ebfeefc725923c16168f5403279eeebbb99e095fb62e5a8"}}