{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:IJDC7QXFCUPRA7XHRMGPSPRZ6K","short_pith_number":"pith:IJDC7QXF","schema_version":"1.0","canonical_sha256":"42462fc2e5151f107ee78b0cf93e39f29e82ee30b59d1ecd8f1f0f4192a7b4f3","source":{"kind":"arxiv","id":"1904.05284","version":2},"attestation_state":"computed","paper":{"title":"Light Scattering from Solid-State Quantum Emitters: Beyond the Atomic Picture","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"quant-ph","authors_text":"Ahsan Nazir, Alistair J. Brash, A. Mark Fox, Benjamin Royall, Catherine L. Phillips, Dara P. S. McCutcheon, Edmund Clarke, Jake Iles-Smith, Jesper M{\\o}rk, John O'Hara, Maurice S. Skolnick","submitted_at":"2019-04-10T16:41:10Z","abstract_excerpt":"Coherent scattering of light by a single quantum emitter is a fundamental process at the heart of many proposed quantum technologies. Unlike atomic systems, solid-state emitters couple to their host lattice by phonons. Using a quantum dot in an optical nanocavity, we resolve these interactions in both time and frequency domains, going beyond the atomic picture to develop a comprehensive model of light scattering from solid-state emitters. We find that even in the presence of a cavity, phonon coupling leads to a sideband that is completely insensitive to excitation conditions, and to a non-mono"},"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":"1904.05284","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2019-04-10T16:41:10Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"6ef51f14b00405444066fb0346e9a8025991403ce3fdffe06a8515f173f5c6bb","abstract_canon_sha256":"455df958e0ba8e8d4469b52b53bbb7eca83debca55c460da789631df2c86af04"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:32:29.825193Z","signature_b64":"voVwFtYqfhGSVLWLNh4IQ9zcKTNCpyoiAFIO2AFo4efy+bUdgSSrMsfrEKpDIq8nLLMf8KdYWG9Zkmjywl97AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"42462fc2e5151f107ee78b0cf93e39f29e82ee30b59d1ecd8f1f0f4192a7b4f3","last_reissued_at":"2026-07-05T00:32:29.824713Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:32:29.824713Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Light Scattering from Solid-State Quantum Emitters: Beyond the Atomic Picture","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"quant-ph","authors_text":"Ahsan Nazir, Alistair J. Brash, A. Mark Fox, Benjamin Royall, Catherine L. Phillips, Dara P. S. McCutcheon, Edmund Clarke, Jake Iles-Smith, Jesper M{\\o}rk, John O'Hara, Maurice S. Skolnick","submitted_at":"2019-04-10T16:41:10Z","abstract_excerpt":"Coherent scattering of light by a single quantum emitter is a fundamental process at the heart of many proposed quantum technologies. Unlike atomic systems, solid-state emitters couple to their host lattice by phonons. Using a quantum dot in an optical nanocavity, we resolve these interactions in both time and frequency domains, going beyond the atomic picture to develop a comprehensive model of light scattering from solid-state emitters. We find that even in the presence of a cavity, phonon coupling leads to a sideband that is completely insensitive to excitation conditions, and to a non-mono"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1904.05284","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1904.05284/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1904.05284","created_at":"2026-07-05T00:32:29.824785+00:00"},{"alias_kind":"arxiv_version","alias_value":"1904.05284v2","created_at":"2026-07-05T00:32:29.824785+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1904.05284","created_at":"2026-07-05T00:32:29.824785+00:00"},{"alias_kind":"pith_short_12","alias_value":"IJDC7QXFCUPR","created_at":"2026-07-05T00:32:29.824785+00:00"},{"alias_kind":"pith_short_16","alias_value":"IJDC7QXFCUPRA7XH","created_at":"2026-07-05T00:32:29.824785+00:00"},{"alias_kind":"pith_short_8","alias_value":"IJDC7QXF","created_at":"2026-07-05T00:32:29.824785+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/IJDC7QXFCUPRA7XHRMGPSPRZ6K","json":"https://pith.science/pith/IJDC7QXFCUPRA7XHRMGPSPRZ6K.json","graph_json":"https://pith.science/api/pith-number/IJDC7QXFCUPRA7XHRMGPSPRZ6K/graph.json","events_json":"https://pith.science/api/pith-number/IJDC7QXFCUPRA7XHRMGPSPRZ6K/events.json","paper":"https://pith.science/paper/IJDC7QXF"},"agent_actions":{"view_html":"https://pith.science/pith/IJDC7QXFCUPRA7XHRMGPSPRZ6K","download_json":"https://pith.science/pith/IJDC7QXFCUPRA7XHRMGPSPRZ6K.json","view_paper":"https://pith.science/paper/IJDC7QXF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1904.05284&json=true","fetch_graph":"https://pith.science/api/pith-number/IJDC7QXFCUPRA7XHRMGPSPRZ6K/graph.json","fetch_events":"https://pith.science/api/pith-number/IJDC7QXFCUPRA7XHRMGPSPRZ6K/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IJDC7QXFCUPRA7XHRMGPSPRZ6K/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IJDC7QXFCUPRA7XHRMGPSPRZ6K/action/storage_attestation","attest_author":"https://pith.science/pith/IJDC7QXFCUPRA7XHRMGPSPRZ6K/action/author_attestation","sign_citation":"https://pith.science/pith/IJDC7QXFCUPRA7XHRMGPSPRZ6K/action/citation_signature","submit_replication":"https://pith.science/pith/IJDC7QXFCUPRA7XHRMGPSPRZ6K/action/replication_record"}},"created_at":"2026-07-05T00:32:29.824785+00:00","updated_at":"2026-07-05T00:32:29.824785+00:00"}