{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:L6A4UEBTA3L5NGCKFOTMXI3NCQ","short_pith_number":"pith:L6A4UEBT","canonical_record":{"source":{"id":"0908.1403","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2009-08-10T20:48:34Z","cross_cats_sorted":[],"title_canon_sha256":"45dfbc964fb3d307ae68867766acc2ead90ba1de87c7910e8f1263befc3e1b2f","abstract_canon_sha256":"91ec959e1ada65fcda3dca99b11d2d577ec3b12f2aa38ea08700a7f38865f8f2"},"schema_version":"1.0"},"canonical_sha256":"5f81ca103306d7d6984a2ba6cba36d14282bab2a69e36c4ac6ff2d4b88636845","source":{"kind":"arxiv","id":"0908.1403","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0908.1403","created_at":"2026-05-18T02:12:35Z"},{"alias_kind":"arxiv_version","alias_value":"0908.1403v1","created_at":"2026-05-18T02:12:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0908.1403","created_at":"2026-05-18T02:12:35Z"},{"alias_kind":"pith_short_12","alias_value":"L6A4UEBTA3L5","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_16","alias_value":"L6A4UEBTA3L5NGCK","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_8","alias_value":"L6A4UEBT","created_at":"2026-05-18T12:26:00Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:L6A4UEBTA3L5NGCKFOTMXI3NCQ","target":"record","payload":{"canonical_record":{"source":{"id":"0908.1403","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2009-08-10T20:48:34Z","cross_cats_sorted":[],"title_canon_sha256":"45dfbc964fb3d307ae68867766acc2ead90ba1de87c7910e8f1263befc3e1b2f","abstract_canon_sha256":"91ec959e1ada65fcda3dca99b11d2d577ec3b12f2aa38ea08700a7f38865f8f2"},"schema_version":"1.0"},"canonical_sha256":"5f81ca103306d7d6984a2ba6cba36d14282bab2a69e36c4ac6ff2d4b88636845","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:12:35.805965Z","signature_b64":"R57mzsBuzgESf9h+ZBeCeuTizYbJMu45opzUD5ErEfRhypS5UUsV0Nen/LQRGk2SBBcQQan7+N7hndmntwNvBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5f81ca103306d7d6984a2ba6cba36d14282bab2a69e36c4ac6ff2d4b88636845","last_reissued_at":"2026-05-18T02:12:35.805209Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:12:35.805209Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0908.1403","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":"2026-05-18T02:12:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3gHvybpRvNTRKPNb0+fFXmx51IpV4RpS/X0F0x2bKBOHE80EM0QbVcKHFZH6OoBS63gz0P8EsGf+amm5IivvCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T04:07:23.099778Z"},"content_sha256":"0594bd10b0e824b17e470713f3596f7d0458c6fcfa763397b7d6d1b02f793226","schema_version":"1.0","event_id":"sha256:0594bd10b0e824b17e470713f3596f7d0458c6fcfa763397b7d6d1b02f793226"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:L6A4UEBTA3L5NGCKFOTMXI3NCQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Transmission function properties for multi-layered structures: Application to super-resolution","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Concita Sibilia, Giuseppe D'Aguanno, Mark J. Bloemer, Michael Scalora, Nadia Mattiucci","submitted_at":"2009-08-10T20:48:34Z","abstract_excerpt":"We discuss the properties of the transmission function in the k-space for a generic multi-layered structure. In particular we analytically demonstrate that a transmission greater than one in the evanescent spectrum (amplification of the evanescent modes) can be directly linked to the guided modes supported by the structure. Moreover we show that the slope of the phase of the transmission function in the propagating spectrum is inversely proportional to the ability of the structure to compensate the diffraction of the propagating modes. We apply these findings to discuss several examples where "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0908.1403","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":"2026-05-18T02:12:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"C8dSYVXUc/bnK3NSv8u/fRp7h1QT6H1y45UsAG1ZlDPU2VJG3x3tBzf3OTPmIMhusucQNGg8+vIlyS0+uD6JDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T04:07:23.100160Z"},"content_sha256":"749a7f7b689e8ca33c808df8535040a96cd4e32504b108738b82957e329c0d05","schema_version":"1.0","event_id":"sha256:749a7f7b689e8ca33c808df8535040a96cd4e32504b108738b82957e329c0d05"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/L6A4UEBTA3L5NGCKFOTMXI3NCQ/bundle.json","state_url":"https://pith.science/pith/L6A4UEBTA3L5NGCKFOTMXI3NCQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/L6A4UEBTA3L5NGCKFOTMXI3NCQ/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":"2026-05-27T04:07:23Z","links":{"resolver":"https://pith.science/pith/L6A4UEBTA3L5NGCKFOTMXI3NCQ","bundle":"https://pith.science/pith/L6A4UEBTA3L5NGCKFOTMXI3NCQ/bundle.json","state":"https://pith.science/pith/L6A4UEBTA3L5NGCKFOTMXI3NCQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/L6A4UEBTA3L5NGCKFOTMXI3NCQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:L6A4UEBTA3L5NGCKFOTMXI3NCQ","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":"91ec959e1ada65fcda3dca99b11d2d577ec3b12f2aa38ea08700a7f38865f8f2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2009-08-10T20:48:34Z","title_canon_sha256":"45dfbc964fb3d307ae68867766acc2ead90ba1de87c7910e8f1263befc3e1b2f"},"schema_version":"1.0","source":{"id":"0908.1403","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0908.1403","created_at":"2026-05-18T02:12:35Z"},{"alias_kind":"arxiv_version","alias_value":"0908.1403v1","created_at":"2026-05-18T02:12:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0908.1403","created_at":"2026-05-18T02:12:35Z"},{"alias_kind":"pith_short_12","alias_value":"L6A4UEBTA3L5","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_16","alias_value":"L6A4UEBTA3L5NGCK","created_at":"2026-05-18T12:26:00Z"},{"alias_kind":"pith_short_8","alias_value":"L6A4UEBT","created_at":"2026-05-18T12:26:00Z"}],"graph_snapshots":[{"event_id":"sha256:749a7f7b689e8ca33c808df8535040a96cd4e32504b108738b82957e329c0d05","target":"graph","created_at":"2026-05-18T02:12:35Z","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 discuss the properties of the transmission function in the k-space for a generic multi-layered structure. In particular we analytically demonstrate that a transmission greater than one in the evanescent spectrum (amplification of the evanescent modes) can be directly linked to the guided modes supported by the structure. Moreover we show that the slope of the phase of the transmission function in the propagating spectrum is inversely proportional to the ability of the structure to compensate the diffraction of the propagating modes. We apply these findings to discuss several examples where ","authors_text":"Concita Sibilia, Giuseppe D'Aguanno, Mark J. Bloemer, Michael Scalora, Nadia Mattiucci","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2009-08-10T20:48:34Z","title":"Transmission function properties for multi-layered structures: Application to super-resolution"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0908.1403","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":"sha256:0594bd10b0e824b17e470713f3596f7d0458c6fcfa763397b7d6d1b02f793226","target":"record","created_at":"2026-05-18T02:12:35Z","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":"91ec959e1ada65fcda3dca99b11d2d577ec3b12f2aa38ea08700a7f38865f8f2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2009-08-10T20:48:34Z","title_canon_sha256":"45dfbc964fb3d307ae68867766acc2ead90ba1de87c7910e8f1263befc3e1b2f"},"schema_version":"1.0","source":{"id":"0908.1403","kind":"arxiv","version":1}},"canonical_sha256":"5f81ca103306d7d6984a2ba6cba36d14282bab2a69e36c4ac6ff2d4b88636845","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5f81ca103306d7d6984a2ba6cba36d14282bab2a69e36c4ac6ff2d4b88636845","first_computed_at":"2026-05-18T02:12:35.805209Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:12:35.805209Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"R57mzsBuzgESf9h+ZBeCeuTizYbJMu45opzUD5ErEfRhypS5UUsV0Nen/LQRGk2SBBcQQan7+N7hndmntwNvBA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:12:35.805965Z","signed_message":"canonical_sha256_bytes"},"source_id":"0908.1403","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0594bd10b0e824b17e470713f3596f7d0458c6fcfa763397b7d6d1b02f793226","sha256:749a7f7b689e8ca33c808df8535040a96cd4e32504b108738b82957e329c0d05"],"state_sha256":"c298e3d3d5c369284b11917b88f16a605fe9ab6d5c9869f2af67d90302595d33"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xW8tLtXP0He3vuMZHccWC5rempOAIY8UUmDBERbCAPTS+O60HuSPERwWSUtARBu1uzMjxBuaMUsR1LnnFV87BQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T04:07:23.102546Z","bundle_sha256":"aa330874030808ec66c2ace791087b62a80e48362332d935a837368b9ed8228c"}}