{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:7I7GRKHOJID7AQ2EOE2VUKDDG6","short_pith_number":"pith:7I7GRKHO","schema_version":"1.0","canonical_sha256":"fa3e68a8ee4a07f0434471355a286337882166ea8e621036014c5f40d86b9aa9","source":{"kind":"arxiv","id":"1711.11490","version":2},"attestation_state":"computed","paper":{"title":"Microscopic theory of cavity-enhanced single-photon emission from optical two-photon Raman processes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Dirk Heinze, Dominik Breddermann, Rolf Binder, Stefan Schumacher, Tom Praschan","submitted_at":"2017-11-30T16:15:48Z","abstract_excerpt":"We consider cavity-enhanced single-photon generation from stimulated two-photon Raman processes in three-level systems. We compare four fundamental system configurations, one $\\Lambda$-, one V- and two ladder ($\\Xi$-) configurations. These can be realized as subsystems of a single quantum dot or of quantum-dot molecules. For a new microscopic understanding of the Raman process, we analyze the Heisenberg equation of motion applying the cluster-expansion scheme. Within this formalism an exact and rigorous definition of a cavity-enhanced Raman photon via its corresponding Raman correlation is pos"},"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":"1711.11490","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-11-30T16:15:48Z","cross_cats_sorted":[],"title_canon_sha256":"1a5e2577900f8bdc0e6ec3d9fd128a3d19c4e39743fea5701e018d42424de48b","abstract_canon_sha256":"348de11419b127e097badcdfffd5f37ce08812cb519079eb2c9196d477468e05"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:21.260439Z","signature_b64":"5SGHn+frONyTn9MPMFZbnz/VU+YjWUDbz0bUWAsgQF9UN7Xk7EyXmPqHIg+vacDdI1Pg1MGjf1T2fXBQO6SvCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fa3e68a8ee4a07f0434471355a286337882166ea8e621036014c5f40d86b9aa9","last_reissued_at":"2026-05-18T00:21:21.258683Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:21.258683Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Microscopic theory of cavity-enhanced single-photon emission from optical two-photon Raman processes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Dirk Heinze, Dominik Breddermann, Rolf Binder, Stefan Schumacher, Tom Praschan","submitted_at":"2017-11-30T16:15:48Z","abstract_excerpt":"We consider cavity-enhanced single-photon generation from stimulated two-photon Raman processes in three-level systems. We compare four fundamental system configurations, one $\\Lambda$-, one V- and two ladder ($\\Xi$-) configurations. These can be realized as subsystems of a single quantum dot or of quantum-dot molecules. For a new microscopic understanding of the Raman process, we analyze the Heisenberg equation of motion applying the cluster-expansion scheme. Within this formalism an exact and rigorous definition of a cavity-enhanced Raman photon via its corresponding Raman correlation is pos"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.11490","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1711.11490","created_at":"2026-05-18T00:21:21.259800+00:00"},{"alias_kind":"arxiv_version","alias_value":"1711.11490v2","created_at":"2026-05-18T00:21:21.259800+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.11490","created_at":"2026-05-18T00:21:21.259800+00:00"},{"alias_kind":"pith_short_12","alias_value":"7I7GRKHOJID7","created_at":"2026-05-18T12:31:05.417338+00:00"},{"alias_kind":"pith_short_16","alias_value":"7I7GRKHOJID7AQ2E","created_at":"2026-05-18T12:31:05.417338+00:00"},{"alias_kind":"pith_short_8","alias_value":"7I7GRKHO","created_at":"2026-05-18T12:31:05.417338+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/7I7GRKHOJID7AQ2EOE2VUKDDG6","json":"https://pith.science/pith/7I7GRKHOJID7AQ2EOE2VUKDDG6.json","graph_json":"https://pith.science/api/pith-number/7I7GRKHOJID7AQ2EOE2VUKDDG6/graph.json","events_json":"https://pith.science/api/pith-number/7I7GRKHOJID7AQ2EOE2VUKDDG6/events.json","paper":"https://pith.science/paper/7I7GRKHO"},"agent_actions":{"view_html":"https://pith.science/pith/7I7GRKHOJID7AQ2EOE2VUKDDG6","download_json":"https://pith.science/pith/7I7GRKHOJID7AQ2EOE2VUKDDG6.json","view_paper":"https://pith.science/paper/7I7GRKHO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1711.11490&json=true","fetch_graph":"https://pith.science/api/pith-number/7I7GRKHOJID7AQ2EOE2VUKDDG6/graph.json","fetch_events":"https://pith.science/api/pith-number/7I7GRKHOJID7AQ2EOE2VUKDDG6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7I7GRKHOJID7AQ2EOE2VUKDDG6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7I7GRKHOJID7AQ2EOE2VUKDDG6/action/storage_attestation","attest_author":"https://pith.science/pith/7I7GRKHOJID7AQ2EOE2VUKDDG6/action/author_attestation","sign_citation":"https://pith.science/pith/7I7GRKHOJID7AQ2EOE2VUKDDG6/action/citation_signature","submit_replication":"https://pith.science/pith/7I7GRKHOJID7AQ2EOE2VUKDDG6/action/replication_record"}},"created_at":"2026-05-18T00:21:21.259800+00:00","updated_at":"2026-05-18T00:21:21.259800+00:00"}