{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:E4AIUEV4NPQRCSJTZWWKNAHVU5","short_pith_number":"pith:E4AIUEV4","canonical_record":{"source":{"id":"1609.04681","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-15T14:52:36Z","cross_cats_sorted":[],"title_canon_sha256":"88897ed864c7c69b70522fdae8dc9e05af78a7c2033efff178c75e0a559b8e99","abstract_canon_sha256":"ed1ddc4de1207feec60f1a8d828d0eb52da2e29f4201d294a12e540f6f12930a"},"schema_version":"1.0"},"canonical_sha256":"27008a12bc6be1114933cdaca680f5a74451acca2241a1bb71b0faa5fb14db21","source":{"kind":"arxiv","id":"1609.04681","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.04681","created_at":"2026-05-18T01:04:35Z"},{"alias_kind":"arxiv_version","alias_value":"1609.04681v1","created_at":"2026-05-18T01:04:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.04681","created_at":"2026-05-18T01:04:35Z"},{"alias_kind":"pith_short_12","alias_value":"E4AIUEV4NPQR","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_16","alias_value":"E4AIUEV4NPQRCSJT","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_8","alias_value":"E4AIUEV4","created_at":"2026-05-18T12:30:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:E4AIUEV4NPQRCSJTZWWKNAHVU5","target":"record","payload":{"canonical_record":{"source":{"id":"1609.04681","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-15T14:52:36Z","cross_cats_sorted":[],"title_canon_sha256":"88897ed864c7c69b70522fdae8dc9e05af78a7c2033efff178c75e0a559b8e99","abstract_canon_sha256":"ed1ddc4de1207feec60f1a8d828d0eb52da2e29f4201d294a12e540f6f12930a"},"schema_version":"1.0"},"canonical_sha256":"27008a12bc6be1114933cdaca680f5a74451acca2241a1bb71b0faa5fb14db21","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:04:35.903558Z","signature_b64":"Jhqz1TAMjs5pix7c/NrSyFrsp+0IGv4vVzqgBJPxlb3qCIazqcHUC/v+bp0Fx+gRGyHFQc1Ep7hyilqcNgUjDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"27008a12bc6be1114933cdaca680f5a74451acca2241a1bb71b0faa5fb14db21","last_reissued_at":"2026-05-18T01:04:35.902801Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:04:35.902801Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1609.04681","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":"2026-05-18T01:04:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PaVAOSovXCtfA8a2HyUEkpUny0IfmC0e17o6INGyee9F1svu0+llSgKuo/zEG9c2ilbDvv8NJSyNiLrNHU4aAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T12:42:27.504100Z"},"content_sha256":"c71eed6da9de2932d1cf3969080beefb5d461b1f7bd748fd43672ec1f8ba6905","schema_version":"1.0","event_id":"sha256:c71eed6da9de2932d1cf3969080beefb5d461b1f7bd748fd43672ec1f8ba6905"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:E4AIUEV4NPQRCSJTZWWKNAHVU5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum Emitters near Layered Plasmonic Nanostructures: Decay Rate Contributions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Anders Pors, Sergey I. Bozhevolnyi","submitted_at":"2016-09-15T14:52:36Z","abstract_excerpt":"We introduce a numerical framework for calculating decay rate contributions when excited two-level quantum emitters are located near layered plasmonic nanostructures, particularly emphasizing the case of plasmonic nanostructures atop metal substrates where three decay channels exist: free space radiation, Ohmic losses, and excitation of surface plasmon polaritons (SPPs). The calculation of decay rate contributions is based on Huygen's equivalence principle together with a near-field to far-field transformation of the local electric field, thereby allowing us to discern the part of the electrom"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.04681","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":"2026-05-18T01:04:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"V6aExx0jc4/U6lTtAAHnY6HBPh7f6HoaFhSyd+83zqer0gMLj7RjABGNG0QkuqKncjXncfCgQtQEZWLW/fBhCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T12:42:27.504477Z"},"content_sha256":"30067b7ee67297c4b1fecf4dbc5aa34b9421f82df7f4a7e1373e056cccf0b25d","schema_version":"1.0","event_id":"sha256:30067b7ee67297c4b1fecf4dbc5aa34b9421f82df7f4a7e1373e056cccf0b25d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/E4AIUEV4NPQRCSJTZWWKNAHVU5/bundle.json","state_url":"https://pith.science/pith/E4AIUEV4NPQRCSJTZWWKNAHVU5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/E4AIUEV4NPQRCSJTZWWKNAHVU5/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":"2026-06-03T12:42:27Z","links":{"resolver":"https://pith.science/pith/E4AIUEV4NPQRCSJTZWWKNAHVU5","bundle":"https://pith.science/pith/E4AIUEV4NPQRCSJTZWWKNAHVU5/bundle.json","state":"https://pith.science/pith/E4AIUEV4NPQRCSJTZWWKNAHVU5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/E4AIUEV4NPQRCSJTZWWKNAHVU5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:E4AIUEV4NPQRCSJTZWWKNAHVU5","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":"ed1ddc4de1207feec60f1a8d828d0eb52da2e29f4201d294a12e540f6f12930a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-15T14:52:36Z","title_canon_sha256":"88897ed864c7c69b70522fdae8dc9e05af78a7c2033efff178c75e0a559b8e99"},"schema_version":"1.0","source":{"id":"1609.04681","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.04681","created_at":"2026-05-18T01:04:35Z"},{"alias_kind":"arxiv_version","alias_value":"1609.04681v1","created_at":"2026-05-18T01:04:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.04681","created_at":"2026-05-18T01:04:35Z"},{"alias_kind":"pith_short_12","alias_value":"E4AIUEV4NPQR","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_16","alias_value":"E4AIUEV4NPQRCSJT","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_8","alias_value":"E4AIUEV4","created_at":"2026-05-18T12:30:12Z"}],"graph_snapshots":[{"event_id":"sha256:30067b7ee67297c4b1fecf4dbc5aa34b9421f82df7f4a7e1373e056cccf0b25d","target":"graph","created_at":"2026-05-18T01:04:35Z","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 introduce a numerical framework for calculating decay rate contributions when excited two-level quantum emitters are located near layered plasmonic nanostructures, particularly emphasizing the case of plasmonic nanostructures atop metal substrates where three decay channels exist: free space radiation, Ohmic losses, and excitation of surface plasmon polaritons (SPPs). The calculation of decay rate contributions is based on Huygen's equivalence principle together with a near-field to far-field transformation of the local electric field, thereby allowing us to discern the part of the electrom","authors_text":"Anders Pors, Sergey I. Bozhevolnyi","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-15T14:52:36Z","title":"Quantum Emitters near Layered Plasmonic Nanostructures: Decay Rate Contributions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.04681","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:c71eed6da9de2932d1cf3969080beefb5d461b1f7bd748fd43672ec1f8ba6905","target":"record","created_at":"2026-05-18T01:04:35Z","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":"ed1ddc4de1207feec60f1a8d828d0eb52da2e29f4201d294a12e540f6f12930a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-15T14:52:36Z","title_canon_sha256":"88897ed864c7c69b70522fdae8dc9e05af78a7c2033efff178c75e0a559b8e99"},"schema_version":"1.0","source":{"id":"1609.04681","kind":"arxiv","version":1}},"canonical_sha256":"27008a12bc6be1114933cdaca680f5a74451acca2241a1bb71b0faa5fb14db21","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"27008a12bc6be1114933cdaca680f5a74451acca2241a1bb71b0faa5fb14db21","first_computed_at":"2026-05-18T01:04:35.902801Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:04:35.902801Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Jhqz1TAMjs5pix7c/NrSyFrsp+0IGv4vVzqgBJPxlb3qCIazqcHUC/v+bp0Fx+gRGyHFQc1Ep7hyilqcNgUjDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:04:35.903558Z","signed_message":"canonical_sha256_bytes"},"source_id":"1609.04681","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c71eed6da9de2932d1cf3969080beefb5d461b1f7bd748fd43672ec1f8ba6905","sha256:30067b7ee67297c4b1fecf4dbc5aa34b9421f82df7f4a7e1373e056cccf0b25d"],"state_sha256":"d4c2f128ef3c68e416d4f60510036036f2362bebca76c58301d82102588a42ac"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wZAV5D+Jj7zJN/I6+A73igPraEXAa5XYOaw0kKbots5bYyI8rEQNtTB+wBwcThHTA8kq/gTyQeOQivdtZvVrAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T12:42:27.506966Z","bundle_sha256":"4c780783d1eefbbb900a4393cc1bfb04ac2621f3c7377402494b2b5ebcc8078e"}}