{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:Q5VNW3OPCLQROLNHXQWOOY5LSH","short_pith_number":"pith:Q5VNW3OP","canonical_record":{"source":{"id":"1609.01099","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-05T11:08:06Z","cross_cats_sorted":[],"title_canon_sha256":"a888aac498d6b651330100bdca58ed31fd04878f52caabba5f438d14945e11a9","abstract_canon_sha256":"67e2865a2d6e0d77fcba5c21b8047631a6a4285b72c9a59c8f94eae962a718d7"},"schema_version":"1.0"},"canonical_sha256":"876adb6dcf12e1172da7bc2ce763ab91e90c11157fe00ce02a266e2e2989b62d","source":{"kind":"arxiv","id":"1609.01099","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.01099","created_at":"2026-05-18T00:50:19Z"},{"alias_kind":"arxiv_version","alias_value":"1609.01099v2","created_at":"2026-05-18T00:50:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.01099","created_at":"2026-05-18T00:50:19Z"},{"alias_kind":"pith_short_12","alias_value":"Q5VNW3OPCLQR","created_at":"2026-05-18T12:30:39Z"},{"alias_kind":"pith_short_16","alias_value":"Q5VNW3OPCLQROLNH","created_at":"2026-05-18T12:30:39Z"},{"alias_kind":"pith_short_8","alias_value":"Q5VNW3OP","created_at":"2026-05-18T12:30:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:Q5VNW3OPCLQROLNHXQWOOY5LSH","target":"record","payload":{"canonical_record":{"source":{"id":"1609.01099","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-05T11:08:06Z","cross_cats_sorted":[],"title_canon_sha256":"a888aac498d6b651330100bdca58ed31fd04878f52caabba5f438d14945e11a9","abstract_canon_sha256":"67e2865a2d6e0d77fcba5c21b8047631a6a4285b72c9a59c8f94eae962a718d7"},"schema_version":"1.0"},"canonical_sha256":"876adb6dcf12e1172da7bc2ce763ab91e90c11157fe00ce02a266e2e2989b62d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:50:19.264341Z","signature_b64":"50myzzPLIR5uRDeqnt56VjNMFTQ+zlnMGOn7rDKh242UACStK78RymYJJ+D9GCH68ap/QAsyXuSVoFWCkBuQDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"876adb6dcf12e1172da7bc2ce763ab91e90c11157fe00ce02a266e2e2989b62d","last_reissued_at":"2026-05-18T00:50:19.263642Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:50:19.263642Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1609.01099","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:50:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+BfY1JMnn6VoLXYUG5WI0iSTMa39Vw0Z+bjtez4dHIaoseoBIHuaked0jwtNlt2cd5GgV3SZvWy3at3Ea36eAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T20:48:36.290612Z"},"content_sha256":"86f6a7ced7aca8ffe291f7576484213000717027e0069e625e70fc57ce818b6d","schema_version":"1.0","event_id":"sha256:86f6a7ced7aca8ffe291f7576484213000717027e0069e625e70fc57ce818b6d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:Q5VNW3OPCLQROLNHXQWOOY5LSH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Multipolar interference effects in nanophotonics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Wei Liu, Yuri S. Kivshar","submitted_at":"2016-09-05T11:08:06Z","abstract_excerpt":"Scattering of electromagnetic waves by an arbitrary nanoscale object can be characterized by a multipole decomposition of the electromagnetic field that allows to describe the scattering intensity and radiation pattern through interferences of dominating excited multipole modes. In modern nanophotonics, both generation and interference of multipole modes start to play an indispensable role, and they enable nanoscale manipulation of light with many related applications. Here we review the multipolar interference effects in metallic, metal-dielectric, and dielectric nanostructures, and suggest a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.01099","kind":"arxiv","version":2},"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":"2026-05-18T00:50:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hCOz1lTicVwj5iUR7RTPUiy2bE0NaAedvuZWVAZdvmiEVjRHm2nxOJAObTxG5VleAw3uA/eFLL/R+uLyse/EDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T20:48:36.291338Z"},"content_sha256":"429bccd4cdc1c778349d314568512e6916ade1960360c9b59822979d476da1e9","schema_version":"1.0","event_id":"sha256:429bccd4cdc1c778349d314568512e6916ade1960360c9b59822979d476da1e9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/Q5VNW3OPCLQROLNHXQWOOY5LSH/bundle.json","state_url":"https://pith.science/pith/Q5VNW3OPCLQROLNHXQWOOY5LSH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/Q5VNW3OPCLQROLNHXQWOOY5LSH/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":"2026-05-27T20:48:36Z","links":{"resolver":"https://pith.science/pith/Q5VNW3OPCLQROLNHXQWOOY5LSH","bundle":"https://pith.science/pith/Q5VNW3OPCLQROLNHXQWOOY5LSH/bundle.json","state":"https://pith.science/pith/Q5VNW3OPCLQROLNHXQWOOY5LSH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/Q5VNW3OPCLQROLNHXQWOOY5LSH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:Q5VNW3OPCLQROLNHXQWOOY5LSH","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":"67e2865a2d6e0d77fcba5c21b8047631a6a4285b72c9a59c8f94eae962a718d7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-05T11:08:06Z","title_canon_sha256":"a888aac498d6b651330100bdca58ed31fd04878f52caabba5f438d14945e11a9"},"schema_version":"1.0","source":{"id":"1609.01099","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.01099","created_at":"2026-05-18T00:50:19Z"},{"alias_kind":"arxiv_version","alias_value":"1609.01099v2","created_at":"2026-05-18T00:50:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.01099","created_at":"2026-05-18T00:50:19Z"},{"alias_kind":"pith_short_12","alias_value":"Q5VNW3OPCLQR","created_at":"2026-05-18T12:30:39Z"},{"alias_kind":"pith_short_16","alias_value":"Q5VNW3OPCLQROLNH","created_at":"2026-05-18T12:30:39Z"},{"alias_kind":"pith_short_8","alias_value":"Q5VNW3OP","created_at":"2026-05-18T12:30:39Z"}],"graph_snapshots":[{"event_id":"sha256:429bccd4cdc1c778349d314568512e6916ade1960360c9b59822979d476da1e9","target":"graph","created_at":"2026-05-18T00:50:19Z","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":"Scattering of electromagnetic waves by an arbitrary nanoscale object can be characterized by a multipole decomposition of the electromagnetic field that allows to describe the scattering intensity and radiation pattern through interferences of dominating excited multipole modes. In modern nanophotonics, both generation and interference of multipole modes start to play an indispensable role, and they enable nanoscale manipulation of light with many related applications. Here we review the multipolar interference effects in metallic, metal-dielectric, and dielectric nanostructures, and suggest a","authors_text":"Wei Liu, Yuri S. Kivshar","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-05T11:08:06Z","title":"Multipolar interference effects in nanophotonics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.01099","kind":"arxiv","version":2},"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":"sha256:86f6a7ced7aca8ffe291f7576484213000717027e0069e625e70fc57ce818b6d","target":"record","created_at":"2026-05-18T00:50:19Z","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":"67e2865a2d6e0d77fcba5c21b8047631a6a4285b72c9a59c8f94eae962a718d7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2016-09-05T11:08:06Z","title_canon_sha256":"a888aac498d6b651330100bdca58ed31fd04878f52caabba5f438d14945e11a9"},"schema_version":"1.0","source":{"id":"1609.01099","kind":"arxiv","version":2}},"canonical_sha256":"876adb6dcf12e1172da7bc2ce763ab91e90c11157fe00ce02a266e2e2989b62d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"876adb6dcf12e1172da7bc2ce763ab91e90c11157fe00ce02a266e2e2989b62d","first_computed_at":"2026-05-18T00:50:19.263642Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:50:19.263642Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"50myzzPLIR5uRDeqnt56VjNMFTQ+zlnMGOn7rDKh242UACStK78RymYJJ+D9GCH68ap/QAsyXuSVoFWCkBuQDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:50:19.264341Z","signed_message":"canonical_sha256_bytes"},"source_id":"1609.01099","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:86f6a7ced7aca8ffe291f7576484213000717027e0069e625e70fc57ce818b6d","sha256:429bccd4cdc1c778349d314568512e6916ade1960360c9b59822979d476da1e9"],"state_sha256":"f4157392bdb84181e65e6aa7b21ce9e8c006a015c7ffa6d77d017f0045f2db6d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8Nta6epmU2JNgcDffxfc19HnhXkaCkUYVs7FHG4dICHLLufbQsA78Rw49TK9PNXOSzbRUrKyZDU7ePTqupS7Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T20:48:36.295058Z","bundle_sha256":"748cd9d72d022c0ba2e7ff0b64fb973600e4be186df22e41cece3e420320492c"}}