{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:FZ5ZXYVUDPJ5XI4ELSD5EMVO2L","short_pith_number":"pith:FZ5ZXYVU","canonical_record":{"source":{"id":"1011.4358","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2010-11-19T08:00:53Z","cross_cats_sorted":[],"title_canon_sha256":"ef0ce2e2d6e887ae5308feda8815e2488b22a998511f841781246e6a9f48de5a","abstract_canon_sha256":"93257bdf3b62a021a6dfe62ab2f24bf9071d61fe7c081335054889326f9fea31"},"schema_version":"1.0"},"canonical_sha256":"2e7b9be2b41bd3dba3845c87d232aed2c5513ebb7d608b95297af26b5b206c42","source":{"kind":"arxiv","id":"1011.4358","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1011.4358","created_at":"2026-05-18T02:04:43Z"},{"alias_kind":"arxiv_version","alias_value":"1011.4358v1","created_at":"2026-05-18T02:04:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.4358","created_at":"2026-05-18T02:04:43Z"},{"alias_kind":"pith_short_12","alias_value":"FZ5ZXYVUDPJ5","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_16","alias_value":"FZ5ZXYVUDPJ5XI4E","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_8","alias_value":"FZ5ZXYVU","created_at":"2026-05-18T12:26:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:FZ5ZXYVUDPJ5XI4ELSD5EMVO2L","target":"record","payload":{"canonical_record":{"source":{"id":"1011.4358","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2010-11-19T08:00:53Z","cross_cats_sorted":[],"title_canon_sha256":"ef0ce2e2d6e887ae5308feda8815e2488b22a998511f841781246e6a9f48de5a","abstract_canon_sha256":"93257bdf3b62a021a6dfe62ab2f24bf9071d61fe7c081335054889326f9fea31"},"schema_version":"1.0"},"canonical_sha256":"2e7b9be2b41bd3dba3845c87d232aed2c5513ebb7d608b95297af26b5b206c42","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:04:43.614528Z","signature_b64":"enbbZqbfj8L1Fq9+xfKLvR3lqucQHBv+M3nMQG3GWu5UFvkcxVB7naDzs/+24+r4BA2/sxKBxUtv5gElzeb8Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2e7b9be2b41bd3dba3845c87d232aed2c5513ebb7d608b95297af26b5b206c42","last_reissued_at":"2026-05-18T02:04:43.613787Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:04:43.613787Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1011.4358","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":"2026-05-18T02:04:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wPSB0tPXfy7QnY3PSV9iDU+3NcYBfYThAu9qRKUo+qMev9SY/Qaz9eGEimICS60kJxlSHZihpywOY0iJT+ZJAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T03:38:13.832787Z"},"content_sha256":"4d5d32ca6d24e23378e77fd9704dd5a70277711d388da3b8681943750828b1b7","schema_version":"1.0","event_id":"sha256:4d5d32ca6d24e23378e77fd9704dd5a70277711d388da3b8681943750828b1b7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:FZ5ZXYVUDPJ5XI4ELSD5EMVO2L","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Plasmonic-dielectric compound grating with high group-index and transmission","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Chun Jiang, Lei Dai, Yang Liu","submitted_at":"2010-11-19T08:00:53Z","abstract_excerpt":"We propose a compound system consisting of a dielectric grating and a plasmonic resonance cavity embedded in the grating. Based on the interference effect between the surface mode supported by the dielectric grating and the plasmonic-induced cavity mode, this system could achieve slow light with group index more than 200 and transmission more than 75%. Meanwhile, we examine the effects of the period numbers of the compound system and photonic crystal superlattice made up of alternate layers of the grating and air on the properties of slow light."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.4358","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":"2026-05-18T02:04:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dH5QFQBygqkf9mAh60QLK9DA00y5vFC8iJeE59+PEixLE3iZ15l7WQQQbNIamdYhR4BG+RL5+r2OnKRhsiU5BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T03:38:13.833144Z"},"content_sha256":"328718614fce0697a4126a20826a23366f7e4e8ecc15baca2cc8b95b648597fb","schema_version":"1.0","event_id":"sha256:328718614fce0697a4126a20826a23366f7e4e8ecc15baca2cc8b95b648597fb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FZ5ZXYVUDPJ5XI4ELSD5EMVO2L/bundle.json","state_url":"https://pith.science/pith/FZ5ZXYVUDPJ5XI4ELSD5EMVO2L/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FZ5ZXYVUDPJ5XI4ELSD5EMVO2L/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":"2026-06-03T03:38:13Z","links":{"resolver":"https://pith.science/pith/FZ5ZXYVUDPJ5XI4ELSD5EMVO2L","bundle":"https://pith.science/pith/FZ5ZXYVUDPJ5XI4ELSD5EMVO2L/bundle.json","state":"https://pith.science/pith/FZ5ZXYVUDPJ5XI4ELSD5EMVO2L/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FZ5ZXYVUDPJ5XI4ELSD5EMVO2L/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:FZ5ZXYVUDPJ5XI4ELSD5EMVO2L","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":"93257bdf3b62a021a6dfe62ab2f24bf9071d61fe7c081335054889326f9fea31","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2010-11-19T08:00:53Z","title_canon_sha256":"ef0ce2e2d6e887ae5308feda8815e2488b22a998511f841781246e6a9f48de5a"},"schema_version":"1.0","source":{"id":"1011.4358","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1011.4358","created_at":"2026-05-18T02:04:43Z"},{"alias_kind":"arxiv_version","alias_value":"1011.4358v1","created_at":"2026-05-18T02:04:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.4358","created_at":"2026-05-18T02:04:43Z"},{"alias_kind":"pith_short_12","alias_value":"FZ5ZXYVUDPJ5","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_16","alias_value":"FZ5ZXYVUDPJ5XI4E","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_8","alias_value":"FZ5ZXYVU","created_at":"2026-05-18T12:26:07Z"}],"graph_snapshots":[{"event_id":"sha256:328718614fce0697a4126a20826a23366f7e4e8ecc15baca2cc8b95b648597fb","target":"graph","created_at":"2026-05-18T02:04:43Z","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 propose a compound system consisting of a dielectric grating and a plasmonic resonance cavity embedded in the grating. Based on the interference effect between the surface mode supported by the dielectric grating and the plasmonic-induced cavity mode, this system could achieve slow light with group index more than 200 and transmission more than 75%. Meanwhile, we examine the effects of the period numbers of the compound system and photonic crystal superlattice made up of alternate layers of the grating and air on the properties of slow light.","authors_text":"Chun Jiang, Lei Dai, Yang Liu","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2010-11-19T08:00:53Z","title":"Plasmonic-dielectric compound grating with high group-index and transmission"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.4358","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":"sha256:4d5d32ca6d24e23378e77fd9704dd5a70277711d388da3b8681943750828b1b7","target":"record","created_at":"2026-05-18T02:04:43Z","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":"93257bdf3b62a021a6dfe62ab2f24bf9071d61fe7c081335054889326f9fea31","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.optics","submitted_at":"2010-11-19T08:00:53Z","title_canon_sha256":"ef0ce2e2d6e887ae5308feda8815e2488b22a998511f841781246e6a9f48de5a"},"schema_version":"1.0","source":{"id":"1011.4358","kind":"arxiv","version":1}},"canonical_sha256":"2e7b9be2b41bd3dba3845c87d232aed2c5513ebb7d608b95297af26b5b206c42","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2e7b9be2b41bd3dba3845c87d232aed2c5513ebb7d608b95297af26b5b206c42","first_computed_at":"2026-05-18T02:04:43.613787Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:04:43.613787Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"enbbZqbfj8L1Fq9+xfKLvR3lqucQHBv+M3nMQG3GWu5UFvkcxVB7naDzs/+24+r4BA2/sxKBxUtv5gElzeb8Cw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:04:43.614528Z","signed_message":"canonical_sha256_bytes"},"source_id":"1011.4358","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4d5d32ca6d24e23378e77fd9704dd5a70277711d388da3b8681943750828b1b7","sha256:328718614fce0697a4126a20826a23366f7e4e8ecc15baca2cc8b95b648597fb"],"state_sha256":"a8e6d6bcbb97594922946b6636429e337deb867d769d07e762df2786f93c60c5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"y68P5j9xBybPPYZAn2HIFf8EfBf2yX8+0x4PkegP0NbMYycQEWAxcUwyh84YDEaZY37C4WvN1Rl+NFV6C90YAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T03:38:13.835122Z","bundle_sha256":"12c02496d4adc7a46199e6f409416aed54fd636ae7a9fe9911a45fbf6e23be42"}}