{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:TQGUAH46ZIDTALTQU2Y7RVNUX3","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"c91023747167ac5a03d45973115323921ef864b356a79d53b8fa1836f02ef7ce","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-12-18T13:42:40Z","title_canon_sha256":"685b4ea8d8c8ede419701286047946fca51668284e95473bca2004f0392da349"},"schema_version":"1.0","source":{"id":"1512.05952","kind":"arxiv","version":5}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.05952","created_at":"2026-05-18T01:00:19Z"},{"alias_kind":"arxiv_version","alias_value":"1512.05952v5","created_at":"2026-05-18T01:00:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.05952","created_at":"2026-05-18T01:00:19Z"},{"alias_kind":"pith_short_12","alias_value":"TQGUAH46ZIDT","created_at":"2026-05-18T12:29:42Z"},{"alias_kind":"pith_short_16","alias_value":"TQGUAH46ZIDTALTQ","created_at":"2026-05-18T12:29:42Z"},{"alias_kind":"pith_short_8","alias_value":"TQGUAH46","created_at":"2026-05-18T12:29:42Z"}],"graph_snapshots":[{"event_id":"sha256:9e8e98fdb7ebbc9f2f6bb66b45ab0930be5922f4d553c31e2f11bfd2a8da1fd4","target":"graph","created_at":"2026-05-18T01:00:19Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Strongly coupled quantum dot-cavity systems provide a non-linear configuration of hybridized light-matter states with promising quantum-optical applications. Here, we investigate the coherent interaction between strong laser pulses and quantum dot-cavity polaritons. Resonant excitation of polaritonic states and their interaction with phonons allow us to observe coherent Rabi oscillations and Ramsey fringes. Furthermore, we demonstrate complete coherent control of a quantum dot-photonic crystal cavity based quantum-bit. By controlling the excitation power and phase in a two-pulse excitation sch","authors_text":"Armand Rundquist, Constantin Dory, Jelena Vuckovic, Jingyuan L. Zhang, Kai M\\\"uller, Kevin A. Fischer, Konstantinos G. Lagoudakis, Tomas Sarmiento, Yousif Kelaita","cross_cats":["physics.optics","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-12-18T13:42:40Z","title":"Complete Coherent Control of a Quantum Dot Strongly Coupled to a Nanocavity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.05952","kind":"arxiv","version":5},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:8bad0092f322abeac85eda446df47aa54cfe73688ed5026d8cb7528fd3430fa8","target":"record","created_at":"2026-05-18T01:00:19Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"c91023747167ac5a03d45973115323921ef864b356a79d53b8fa1836f02ef7ce","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-12-18T13:42:40Z","title_canon_sha256":"685b4ea8d8c8ede419701286047946fca51668284e95473bca2004f0392da349"},"schema_version":"1.0","source":{"id":"1512.05952","kind":"arxiv","version":5}},"canonical_sha256":"9c0d401f9eca07302e70a6b1f8d5b4bef3b2a92bfc1e0987df4438e66b2fd0ab","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9c0d401f9eca07302e70a6b1f8d5b4bef3b2a92bfc1e0987df4438e66b2fd0ab","first_computed_at":"2026-05-18T01:00:19.600132Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:00:19.600132Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"oiqKjDTWvUQg0Ye42RZHH4XKthel0JDPfBmwpg4qV5xRYQpemAd1SulV6HTpvi08SAOu17eWsa1WQ3EIjTcaAA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:00:19.600807Z","signed_message":"canonical_sha256_bytes"},"source_id":"1512.05952","source_kind":"arxiv","source_version":5}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8bad0092f322abeac85eda446df47aa54cfe73688ed5026d8cb7528fd3430fa8","sha256:9e8e98fdb7ebbc9f2f6bb66b45ab0930be5922f4d553c31e2f11bfd2a8da1fd4"],"state_sha256":"fdccfa5d3c942b7912e99bf5248f881fd60477fd9fb46764b9a02f2458b23d99"}