{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:A55PRQMMUDMAGNHJLPNILE6TKK","short_pith_number":"pith:A55PRQMM","schema_version":"1.0","canonical_sha256":"077af8c18ca0d80334e95bda8593d352815e0a2e4d130881a15e6d56068d2a5b","source":{"kind":"arxiv","id":"1610.04129","version":1},"attestation_state":"computed","paper":{"title":"Emission from quantum-dot high- microcavities: transition from spontaneous emission to lasing and the effects of superradiant emitter coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"C. Gies, C. Schneider, F. Jahnke, J. Wolters, M. Kamp, S. H\\\"ofling, S. Kreinberg, S. Reitzenstein, W. W. Chow","submitted_at":"2016-10-13T15:31:07Z","abstract_excerpt":"Measured and calculated results are presented on the emission properties of a new class of emitters operating in the cavity quantum electrodynamics regime. The structures are based on high-finesse GaAs/AlAs micropillar cavities, each with an active medium consisting of a layer of InGaAs quantum dots and distinguishing feature of having substantial fraction of spontaneous emission channeled into one cavity mode (high-beta factor). This paper shows that the usual criterion for lasing with a conventional (low-beta factor) cavity, a sharp nonlinearity in an input-output curve accompanied by notice"},"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":"1610.04129","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-10-13T15:31:07Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"07cae3c907d6cf5334dd0cc7ecd09496802e310a260d1a6bdb4f5c6fa4103463","abstract_canon_sha256":"e1dac4b4c44d860f96b0bc6ecf23efbeadee8dcc407e484dc64f2dc40d19709b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:26:51.952454Z","signature_b64":"GmnXTkAP6VFqBRo2OKwBcx/S6DtREl9MNEM5CNv25p1nQGMIMTiQXoHYkRwiBS0lxNoW69t/W3iw5bbHrMb1CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"077af8c18ca0d80334e95bda8593d352815e0a2e4d130881a15e6d56068d2a5b","last_reissued_at":"2026-05-18T00:26:51.951747Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:26:51.951747Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Emission from quantum-dot high- microcavities: transition from spontaneous emission to lasing and the effects of superradiant emitter coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"C. Gies, C. Schneider, F. Jahnke, J. Wolters, M. Kamp, S. H\\\"ofling, S. Kreinberg, S. Reitzenstein, W. W. Chow","submitted_at":"2016-10-13T15:31:07Z","abstract_excerpt":"Measured and calculated results are presented on the emission properties of a new class of emitters operating in the cavity quantum electrodynamics regime. The structures are based on high-finesse GaAs/AlAs micropillar cavities, each with an active medium consisting of a layer of InGaAs quantum dots and distinguishing feature of having substantial fraction of spontaneous emission channeled into one cavity mode (high-beta factor). This paper shows that the usual criterion for lasing with a conventional (low-beta factor) cavity, a sharp nonlinearity in an input-output curve accompanied by notice"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.04129","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":"1610.04129","created_at":"2026-05-18T00:26:51.951852+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.04129v1","created_at":"2026-05-18T00:26:51.951852+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.04129","created_at":"2026-05-18T00:26:51.951852+00:00"},{"alias_kind":"pith_short_12","alias_value":"A55PRQMMUDMA","created_at":"2026-05-18T12:30:04.600751+00:00"},{"alias_kind":"pith_short_16","alias_value":"A55PRQMMUDMAGNHJ","created_at":"2026-05-18T12:30:04.600751+00:00"},{"alias_kind":"pith_short_8","alias_value":"A55PRQMM","created_at":"2026-05-18T12:30:04.600751+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/A55PRQMMUDMAGNHJLPNILE6TKK","json":"https://pith.science/pith/A55PRQMMUDMAGNHJLPNILE6TKK.json","graph_json":"https://pith.science/api/pith-number/A55PRQMMUDMAGNHJLPNILE6TKK/graph.json","events_json":"https://pith.science/api/pith-number/A55PRQMMUDMAGNHJLPNILE6TKK/events.json","paper":"https://pith.science/paper/A55PRQMM"},"agent_actions":{"view_html":"https://pith.science/pith/A55PRQMMUDMAGNHJLPNILE6TKK","download_json":"https://pith.science/pith/A55PRQMMUDMAGNHJLPNILE6TKK.json","view_paper":"https://pith.science/paper/A55PRQMM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.04129&json=true","fetch_graph":"https://pith.science/api/pith-number/A55PRQMMUDMAGNHJLPNILE6TKK/graph.json","fetch_events":"https://pith.science/api/pith-number/A55PRQMMUDMAGNHJLPNILE6TKK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/A55PRQMMUDMAGNHJLPNILE6TKK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/A55PRQMMUDMAGNHJLPNILE6TKK/action/storage_attestation","attest_author":"https://pith.science/pith/A55PRQMMUDMAGNHJLPNILE6TKK/action/author_attestation","sign_citation":"https://pith.science/pith/A55PRQMMUDMAGNHJLPNILE6TKK/action/citation_signature","submit_replication":"https://pith.science/pith/A55PRQMMUDMAGNHJLPNILE6TKK/action/replication_record"}},"created_at":"2026-05-18T00:26:51.951852+00:00","updated_at":"2026-05-18T00:26:51.951852+00:00"}