{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:SQK3VSVNIAXX5YVNRD6463MHOP","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":"893b1f629e7fe57cb3953c2895fabf60a577d80a8ef843c5ccc721f877267504","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-01-05T13:15:09Z","title_canon_sha256":"bcb88b7ceccd070bc5676b92dacc242f4ceed2c972b9c2f8f4d8191c8b25747b"},"schema_version":"1.0","source":{"id":"1701.01304","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1701.01304","created_at":"2026-05-18T00:40:59Z"},{"alias_kind":"arxiv_version","alias_value":"1701.01304v2","created_at":"2026-05-18T00:40:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.01304","created_at":"2026-05-18T00:40:59Z"},{"alias_kind":"pith_short_12","alias_value":"SQK3VSVNIAXX","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_16","alias_value":"SQK3VSVNIAXX5YVN","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_8","alias_value":"SQK3VSVN","created_at":"2026-05-18T12:31:43Z"}],"graph_snapshots":[{"event_id":"sha256:282da9073d718649f609fa1d2f98a5138948b2f1e76654a8f1cb3234e379458e","target":"graph","created_at":"2026-05-18T00:40:59Z","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":"Excitation of a semiconductor quantum dot with a chirped laser pulse allows excitons to be created by rapid adiabatic passage. In quantum dots this process can be greatly hindered by the coupling to phonons. Here we add a high chirp rate to ultra-short laser pulses and use these pulses to excite a single quantum dot. We demonstrate that we enter a regime where the exciton-phonon coupling is effective for small pulse areas, while for higher pulse areas a decoupling of the exciton from the phonons occurs. We thus discover a reappearance of rapid adiabatic passage, in analogy to the predicted rea","authors_text":"(2) Institut f\\\"ur Festk\\\"orpertheorie, 3), (3) IBM Research-Zurich, (4) Lehrstuhl f\\\"ur Angewandte Festk\\\"orperphysik, (5) Universit\\'e C\\^ote d'Azur, Andreas D. Wieck (4), Andreas V. Kuhlmann (1, Arne Ludwig (4), CNRS, CRHEA, Doris E. Reiter (2), France), Germany, Jean-Michel Chauveau (5), Richard J. Warburton (1) ((1) Department of Physics, Ruhr-Universit\\\"at Bochum, Sascha R. Valentin (4), Sebastian L\\\"uker (2), Switzerland, Tilmann Kuhn (2), Timo Kaldewey (1), Universit\\\"at M\\\"unster, University of Basel","cross_cats":["physics.optics","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-01-05T13:15:09Z","title":"Demonstrating the decoupling regime of the electron-phonon interaction in a quantum dot using chirped optical excitation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.01304","kind":"arxiv","version":2},"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":"sha256:8a84a89a50111a963ac70159e1a0f737f3acbb1513203b070b993a4e293904fb","target":"record","created_at":"2026-05-18T00:40:59Z","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":"893b1f629e7fe57cb3953c2895fabf60a577d80a8ef843c5ccc721f877267504","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-01-05T13:15:09Z","title_canon_sha256":"bcb88b7ceccd070bc5676b92dacc242f4ceed2c972b9c2f8f4d8191c8b25747b"},"schema_version":"1.0","source":{"id":"1701.01304","kind":"arxiv","version":2}},"canonical_sha256":"9415bacaad402f7ee2ad88fdcf6d8773ed1369e27657a192735532e27f25e1f7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9415bacaad402f7ee2ad88fdcf6d8773ed1369e27657a192735532e27f25e1f7","first_computed_at":"2026-05-18T00:40:59.250000Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:40:59.250000Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZicJb4CBTDyy6p6ITPsUJrTXPX8pForQ1ez+UhCRD5HAPz3JUzt/2uK6d4fR7G+ICdNglp9YXxc4gFIEADcABg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:40:59.250544Z","signed_message":"canonical_sha256_bytes"},"source_id":"1701.01304","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8a84a89a50111a963ac70159e1a0f737f3acbb1513203b070b993a4e293904fb","sha256:282da9073d718649f609fa1d2f98a5138948b2f1e76654a8f1cb3234e379458e"],"state_sha256":"8957481d349602f5227a0016232564808c38e2987f8bedecee00d9f4283d64f4"}