{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:2H4X3K5C4ZC377BRXV5S2OXGFH","short_pith_number":"pith:2H4X3K5C","schema_version":"1.0","canonical_sha256":"d1f97daba2e645bffc31bd7b2d3ae629d165579c9ef759eb6451b3b189bb666c","source":{"kind":"arxiv","id":"1711.05011","version":3},"attestation_state":"computed","paper":{"title":"Rigorous modal analysis of plasmonic nanoresonators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Philippe Lalanne, R\\'emi Faggiani, Wei Yan","submitted_at":"2017-11-14T09:26:05Z","abstract_excerpt":"The specificity of modal-expansion formalisms is their capabilities to model the physical properties in the natural resonance-state basis of the system in question, leading to a transparent interpretation of the numerical results. In electromagnetism, modal-expansion formalisms are routinely used for optical waveguides. In contrast, they are much less mature for analyzing open non-Hermitian systems, such as micro and nanoresonators. Here, by accounting for material dispersion with auxiliary fields, we considerably extend the capabilities of these formalisms, in terms of computational effective"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1711.05011","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-11-14T09:26:05Z","cross_cats_sorted":[],"title_canon_sha256":"8fe90cb7f3ed35c72e9dff30b1a26910b9f6d282d62283d832b80033a5b34308","abstract_canon_sha256":"763c8250752d99e0b129a3d33835b99672ae3401c832d74a3cf9c3ceae8c860d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:06:30.908610Z","signature_b64":"5nHl049vLBbG2Qrrjs9fBwjrb+N5E5+SjP+xpUpq3FeFcJYLTgoZZr4+19GupCYjfd49nxsllfn2VN9fwh/6Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d1f97daba2e645bffc31bd7b2d3ae629d165579c9ef759eb6451b3b189bb666c","last_reissued_at":"2026-05-18T00:06:30.908204Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:06:30.908204Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Rigorous modal analysis of plasmonic nanoresonators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Philippe Lalanne, R\\'emi Faggiani, Wei Yan","submitted_at":"2017-11-14T09:26:05Z","abstract_excerpt":"The specificity of modal-expansion formalisms is their capabilities to model the physical properties in the natural resonance-state basis of the system in question, leading to a transparent interpretation of the numerical results. In electromagnetism, modal-expansion formalisms are routinely used for optical waveguides. In contrast, they are much less mature for analyzing open non-Hermitian systems, such as micro and nanoresonators. Here, by accounting for material dispersion with auxiliary fields, we considerably extend the capabilities of these formalisms, in terms of computational effective"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.05011","kind":"arxiv","version":3},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1711.05011","created_at":"2026-05-18T00:06:30.908262+00:00"},{"alias_kind":"arxiv_version","alias_value":"1711.05011v3","created_at":"2026-05-18T00:06:30.908262+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.05011","created_at":"2026-05-18T00:06:30.908262+00:00"},{"alias_kind":"pith_short_12","alias_value":"2H4X3K5C4ZC3","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_16","alias_value":"2H4X3K5C4ZC377BR","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_8","alias_value":"2H4X3K5C","created_at":"2026-05-18T12:30:55.937587+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2H4X3K5C4ZC377BRXV5S2OXGFH","json":"https://pith.science/pith/2H4X3K5C4ZC377BRXV5S2OXGFH.json","graph_json":"https://pith.science/api/pith-number/2H4X3K5C4ZC377BRXV5S2OXGFH/graph.json","events_json":"https://pith.science/api/pith-number/2H4X3K5C4ZC377BRXV5S2OXGFH/events.json","paper":"https://pith.science/paper/2H4X3K5C"},"agent_actions":{"view_html":"https://pith.science/pith/2H4X3K5C4ZC377BRXV5S2OXGFH","download_json":"https://pith.science/pith/2H4X3K5C4ZC377BRXV5S2OXGFH.json","view_paper":"https://pith.science/paper/2H4X3K5C","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1711.05011&json=true","fetch_graph":"https://pith.science/api/pith-number/2H4X3K5C4ZC377BRXV5S2OXGFH/graph.json","fetch_events":"https://pith.science/api/pith-number/2H4X3K5C4ZC377BRXV5S2OXGFH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2H4X3K5C4ZC377BRXV5S2OXGFH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2H4X3K5C4ZC377BRXV5S2OXGFH/action/storage_attestation","attest_author":"https://pith.science/pith/2H4X3K5C4ZC377BRXV5S2OXGFH/action/author_attestation","sign_citation":"https://pith.science/pith/2H4X3K5C4ZC377BRXV5S2OXGFH/action/citation_signature","submit_replication":"https://pith.science/pith/2H4X3K5C4ZC377BRXV5S2OXGFH/action/replication_record"}},"created_at":"2026-05-18T00:06:30.908262+00:00","updated_at":"2026-05-18T00:06:30.908262+00:00"}