{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:GVYOLADN7XCSX63LXL4NLHNRSF","short_pith_number":"pith:GVYOLADN","schema_version":"1.0","canonical_sha256":"3570e5806dfdc52bfb6bbaf8d59db1915e8514858d1824afda6e6852b3c4ab7f","source":{"kind":"arxiv","id":"1312.5769","version":1},"attestation_state":"computed","paper":{"title":"Modes and Mode Volumes of Leaky Optical Cavities and Plasmonic Nanoresonators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Philip Tr{\\o}st Kristensen, Stephen Hughes","submitted_at":"2013-12-19T22:14:27Z","abstract_excerpt":"Electromagnetic cavity modes in photonic and plasmonic resonators offer rich and attractive regimes for tailoring the properties of light-matter interactions. Yet there is a disturbing lack of a precise definition for what constitutes a cavity mode, and as a result their mathematical properties remain largely unspecified. The lack of a definition is evidenced in part by the diverse nomenclature at use - \"resonance\", \"leaky mode\", \"quasimode\", to name but a few - suggesting that the dissipative nature of cavity modes somehow makes them different from other modes, but an explicit distinction is "},"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":"1312.5769","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-12-19T22:14:27Z","cross_cats_sorted":["physics.optics","quant-ph"],"title_canon_sha256":"50f9ddf69b3f2e733c7ec352cbee1ca02ed99a2357c81436c67f61aa29956d36","abstract_canon_sha256":"1e671d49a776b181e8a93a3eda9815b6f1b9df173e0fd07846cc070bc91333a1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:04:07.889352Z","signature_b64":"NiCo1QoMksfxq/Fn0y/OiZmtZd/fuMYeTkKEt0nf/nVaqdOFOmLBsXvboxt6+3gxiNfQriMH7RzDZoM+BYkUAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3570e5806dfdc52bfb6bbaf8d59db1915e8514858d1824afda6e6852b3c4ab7f","last_reissued_at":"2026-05-18T03:04:07.888632Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:04:07.888632Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Modes and Mode Volumes of Leaky Optical Cavities and Plasmonic Nanoresonators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Philip Tr{\\o}st Kristensen, Stephen Hughes","submitted_at":"2013-12-19T22:14:27Z","abstract_excerpt":"Electromagnetic cavity modes in photonic and plasmonic resonators offer rich and attractive regimes for tailoring the properties of light-matter interactions. Yet there is a disturbing lack of a precise definition for what constitutes a cavity mode, and as a result their mathematical properties remain largely unspecified. The lack of a definition is evidenced in part by the diverse nomenclature at use - \"resonance\", \"leaky mode\", \"quasimode\", to name but a few - suggesting that the dissipative nature of cavity modes somehow makes them different from other modes, but an explicit distinction is "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.5769","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1312.5769","created_at":"2026-05-18T03:04:07.888742+00:00"},{"alias_kind":"arxiv_version","alias_value":"1312.5769v1","created_at":"2026-05-18T03:04:07.888742+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.5769","created_at":"2026-05-18T03:04:07.888742+00:00"},{"alias_kind":"pith_short_12","alias_value":"GVYOLADN7XCS","created_at":"2026-05-18T12:27:45.050594+00:00"},{"alias_kind":"pith_short_16","alias_value":"GVYOLADN7XCSX63L","created_at":"2026-05-18T12:27:45.050594+00:00"},{"alias_kind":"pith_short_8","alias_value":"GVYOLADN","created_at":"2026-05-18T12:27:45.050594+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/GVYOLADN7XCSX63LXL4NLHNRSF","json":"https://pith.science/pith/GVYOLADN7XCSX63LXL4NLHNRSF.json","graph_json":"https://pith.science/api/pith-number/GVYOLADN7XCSX63LXL4NLHNRSF/graph.json","events_json":"https://pith.science/api/pith-number/GVYOLADN7XCSX63LXL4NLHNRSF/events.json","paper":"https://pith.science/paper/GVYOLADN"},"agent_actions":{"view_html":"https://pith.science/pith/GVYOLADN7XCSX63LXL4NLHNRSF","download_json":"https://pith.science/pith/GVYOLADN7XCSX63LXL4NLHNRSF.json","view_paper":"https://pith.science/paper/GVYOLADN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1312.5769&json=true","fetch_graph":"https://pith.science/api/pith-number/GVYOLADN7XCSX63LXL4NLHNRSF/graph.json","fetch_events":"https://pith.science/api/pith-number/GVYOLADN7XCSX63LXL4NLHNRSF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GVYOLADN7XCSX63LXL4NLHNRSF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GVYOLADN7XCSX63LXL4NLHNRSF/action/storage_attestation","attest_author":"https://pith.science/pith/GVYOLADN7XCSX63LXL4NLHNRSF/action/author_attestation","sign_citation":"https://pith.science/pith/GVYOLADN7XCSX63LXL4NLHNRSF/action/citation_signature","submit_replication":"https://pith.science/pith/GVYOLADN7XCSX63LXL4NLHNRSF/action/replication_record"}},"created_at":"2026-05-18T03:04:07.888742+00:00","updated_at":"2026-05-18T03:04:07.888742+00:00"}