{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:HQG4XRCFBGQEIU4CU2G3TFHE3M","short_pith_number":"pith:HQG4XRCF","schema_version":"1.0","canonical_sha256":"3c0dcbc44509a0445382a68db994e4db23d21e25be29685ba0473020476b470e","source":{"kind":"arxiv","id":"1803.04941","version":1},"attestation_state":"computed","paper":{"title":"Comparative study of plasmonic antennas for strong coupling and quantum nonlinearities with single emitters","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Benjamin Rousseaux, Denis G. Baranov, G\\\"oran Johansson, Mikael K\\\"all, Timur Shegai","submitted_at":"2018-03-13T17:16:12Z","abstract_excerpt":"Realizing strong coupling between a single quantum emitter (QE) and an optical cavity is of crucial importance in the context of various quantum optical applications. While Rabi splitting of single quantum emitters coupled to high-Q diffraction limited cavities have been reported in numerous configurations, attaining single emitter Rabi splitting with a plasmonic nanostructure is still elusive. Here, we establish the analytical condition for strong coupling between a single QE and a plasmonic nanocavity and apply it to study various plasmonic arrangements that were shown to enable Rabi splitti"},"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":"1803.04941","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2018-03-13T17:16:12Z","cross_cats_sorted":[],"title_canon_sha256":"685026aad06fa74bf1f85040c55866036955a854d9689cf1d00b4716c1bfe575","abstract_canon_sha256":"6739b55aa5696e9d669e5125f1ec8616b7c846fdeed63b31f2d378430260998b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:08:43.032158Z","signature_b64":"cZh9oGXSWCc48BLQ5UB7tnzO/iAf7nMV/9WKvJK9zA8ZFmu1CGpeZ8Y7wOXqXE3FqknN2ZpB/ERyR9qiz4T+CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3c0dcbc44509a0445382a68db994e4db23d21e25be29685ba0473020476b470e","last_reissued_at":"2026-05-18T00:08:43.031461Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:08:43.031461Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Comparative study of plasmonic antennas for strong coupling and quantum nonlinearities with single emitters","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Benjamin Rousseaux, Denis G. Baranov, G\\\"oran Johansson, Mikael K\\\"all, Timur Shegai","submitted_at":"2018-03-13T17:16:12Z","abstract_excerpt":"Realizing strong coupling between a single quantum emitter (QE) and an optical cavity is of crucial importance in the context of various quantum optical applications. While Rabi splitting of single quantum emitters coupled to high-Q diffraction limited cavities have been reported in numerous configurations, attaining single emitter Rabi splitting with a plasmonic nanostructure is still elusive. Here, we establish the analytical condition for strong coupling between a single QE and a plasmonic nanocavity and apply it to study various plasmonic arrangements that were shown to enable Rabi splitti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.04941","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":"1803.04941","created_at":"2026-05-18T00:08:43.031569+00:00"},{"alias_kind":"arxiv_version","alias_value":"1803.04941v1","created_at":"2026-05-18T00:08:43.031569+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.04941","created_at":"2026-05-18T00:08:43.031569+00:00"},{"alias_kind":"pith_short_12","alias_value":"HQG4XRCFBGQE","created_at":"2026-05-18T12:32:28.185984+00:00"},{"alias_kind":"pith_short_16","alias_value":"HQG4XRCFBGQEIU4C","created_at":"2026-05-18T12:32:28.185984+00:00"},{"alias_kind":"pith_short_8","alias_value":"HQG4XRCF","created_at":"2026-05-18T12:32:28.185984+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/HQG4XRCFBGQEIU4CU2G3TFHE3M","json":"https://pith.science/pith/HQG4XRCFBGQEIU4CU2G3TFHE3M.json","graph_json":"https://pith.science/api/pith-number/HQG4XRCFBGQEIU4CU2G3TFHE3M/graph.json","events_json":"https://pith.science/api/pith-number/HQG4XRCFBGQEIU4CU2G3TFHE3M/events.json","paper":"https://pith.science/paper/HQG4XRCF"},"agent_actions":{"view_html":"https://pith.science/pith/HQG4XRCFBGQEIU4CU2G3TFHE3M","download_json":"https://pith.science/pith/HQG4XRCFBGQEIU4CU2G3TFHE3M.json","view_paper":"https://pith.science/paper/HQG4XRCF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1803.04941&json=true","fetch_graph":"https://pith.science/api/pith-number/HQG4XRCFBGQEIU4CU2G3TFHE3M/graph.json","fetch_events":"https://pith.science/api/pith-number/HQG4XRCFBGQEIU4CU2G3TFHE3M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HQG4XRCFBGQEIU4CU2G3TFHE3M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HQG4XRCFBGQEIU4CU2G3TFHE3M/action/storage_attestation","attest_author":"https://pith.science/pith/HQG4XRCFBGQEIU4CU2G3TFHE3M/action/author_attestation","sign_citation":"https://pith.science/pith/HQG4XRCFBGQEIU4CU2G3TFHE3M/action/citation_signature","submit_replication":"https://pith.science/pith/HQG4XRCFBGQEIU4CU2G3TFHE3M/action/replication_record"}},"created_at":"2026-05-18T00:08:43.031569+00:00","updated_at":"2026-05-18T00:08:43.031569+00:00"}