{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:KUJFT6Q564ZGRKKL6HUCP3XSLM","short_pith_number":"pith:KUJFT6Q5","canonical_record":{"source":{"id":"1310.4604","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-17T07:50:43Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"3db149678fbc1475a9794e61e635c73a552a117c9d17faa08ad5387c4d733329","abstract_canon_sha256":"245ec70bf82b2b9fbae369bfe564a34d4ca11018b6699e745c5c09d7ae28c068"},"schema_version":"1.0"},"canonical_sha256":"551259fa1df73268a94bf1e827eef25b3e7644d615f475db86d6392a9a059661","source":{"kind":"arxiv","id":"1310.4604","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.4604","created_at":"2026-05-18T01:46:58Z"},{"alias_kind":"arxiv_version","alias_value":"1310.4604v1","created_at":"2026-05-18T01:46:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.4604","created_at":"2026-05-18T01:46:58Z"},{"alias_kind":"pith_short_12","alias_value":"KUJFT6Q564ZG","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_16","alias_value":"KUJFT6Q564ZGRKKL","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_8","alias_value":"KUJFT6Q5","created_at":"2026-05-18T12:27:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:KUJFT6Q564ZGRKKL6HUCP3XSLM","target":"record","payload":{"canonical_record":{"source":{"id":"1310.4604","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-17T07:50:43Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"3db149678fbc1475a9794e61e635c73a552a117c9d17faa08ad5387c4d733329","abstract_canon_sha256":"245ec70bf82b2b9fbae369bfe564a34d4ca11018b6699e745c5c09d7ae28c068"},"schema_version":"1.0"},"canonical_sha256":"551259fa1df73268a94bf1e827eef25b3e7644d615f475db86d6392a9a059661","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:46:58.558052Z","signature_b64":"jEni4Tho+d2Megi00xmy9i4f8hjFCli3n/qIqjOeLFA/5LZZdqEEFpOu7r57E8rg5VHSU6lPHWdBqB7ExuifBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"551259fa1df73268a94bf1e827eef25b3e7644d615f475db86d6392a9a059661","last_reissued_at":"2026-05-18T01:46:58.557534Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:46:58.557534Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1310.4604","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:46:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lol9pooLQvNNc53d4yTdusFkY6VSixN0Yxxzlk3bmfkJ5q/Cw8ynpn8ftQBKuc4TIulEhUXQH1xeu4m7wY4jCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T22:18:49.306221Z"},"content_sha256":"cd2919e91630034748cba77a7cd8ab67bd296924319273e0de10b0f208017e3e","schema_version":"1.0","event_id":"sha256:cd2919e91630034748cba77a7cd8ab67bd296924319273e0de10b0f208017e3e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:KUJFT6Q564ZGRKKL6HUCP3XSLM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Effects of spontaneously generated coherence on resonance fluorescence from lateral triple quantum -dot molecules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"Chun-Liang Wang, Cun-Zhu Tong, Li-Jun Wang, Si-Cong Tian, Yong-Qiang Ning","submitted_at":"2013-10-17T07:50:43Z","abstract_excerpt":"We investigate the spectrum of the resonance fluorescence from the lateral triple quantum dots controlled by voltage and obtain some interesting features such as controllable triple narrow peaks. In our system we use tunneling instead of coupling lasers, and the positions, widths and heights of the resonance fluorescence peaks can be controlled by tuning the tunneling couplings. We explain the observed spectrum with the transition properties of the dressed states generated by the coupling of the two tunneling and the laser field. These features can also be viewed as the effects of Spontaneousl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.4604","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:46:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CvzhfbUSf3lcsxm5wyVAz5fLGeyor6Tzp9rmyGVr3PL9QZJt7BnTWvlEe2/REWhcUV8F+upoGU6KL/z1/nsCAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T22:18:49.306585Z"},"content_sha256":"b8c132ff0a4a6438452f3370ac9ba08ba030ce7ee55b3a41dc99cec9fea6308b","schema_version":"1.0","event_id":"sha256:b8c132ff0a4a6438452f3370ac9ba08ba030ce7ee55b3a41dc99cec9fea6308b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KUJFT6Q564ZGRKKL6HUCP3XSLM/bundle.json","state_url":"https://pith.science/pith/KUJFT6Q564ZGRKKL6HUCP3XSLM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KUJFT6Q564ZGRKKL6HUCP3XSLM/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-02T22:18:49Z","links":{"resolver":"https://pith.science/pith/KUJFT6Q564ZGRKKL6HUCP3XSLM","bundle":"https://pith.science/pith/KUJFT6Q564ZGRKKL6HUCP3XSLM/bundle.json","state":"https://pith.science/pith/KUJFT6Q564ZGRKKL6HUCP3XSLM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KUJFT6Q564ZGRKKL6HUCP3XSLM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:KUJFT6Q564ZGRKKL6HUCP3XSLM","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":"245ec70bf82b2b9fbae369bfe564a34d4ca11018b6699e745c5c09d7ae28c068","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-17T07:50:43Z","title_canon_sha256":"3db149678fbc1475a9794e61e635c73a552a117c9d17faa08ad5387c4d733329"},"schema_version":"1.0","source":{"id":"1310.4604","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.4604","created_at":"2026-05-18T01:46:58Z"},{"alias_kind":"arxiv_version","alias_value":"1310.4604v1","created_at":"2026-05-18T01:46:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.4604","created_at":"2026-05-18T01:46:58Z"},{"alias_kind":"pith_short_12","alias_value":"KUJFT6Q564ZG","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_16","alias_value":"KUJFT6Q564ZGRKKL","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_8","alias_value":"KUJFT6Q5","created_at":"2026-05-18T12:27:51Z"}],"graph_snapshots":[{"event_id":"sha256:b8c132ff0a4a6438452f3370ac9ba08ba030ce7ee55b3a41dc99cec9fea6308b","target":"graph","created_at":"2026-05-18T01:46:58Z","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":"We investigate the spectrum of the resonance fluorescence from the lateral triple quantum dots controlled by voltage and obtain some interesting features such as controllable triple narrow peaks. In our system we use tunneling instead of coupling lasers, and the positions, widths and heights of the resonance fluorescence peaks can be controlled by tuning the tunneling couplings. We explain the observed spectrum with the transition properties of the dressed states generated by the coupling of the two tunneling and the laser field. These features can also be viewed as the effects of Spontaneousl","authors_text":"Chun-Liang Wang, Cun-Zhu Tong, Li-Jun Wang, Si-Cong Tian, Yong-Qiang Ning","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-17T07:50:43Z","title":"Effects of spontaneously generated coherence on resonance fluorescence from lateral triple quantum -dot molecules"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.4604","kind":"arxiv","version":1},"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:cd2919e91630034748cba77a7cd8ab67bd296924319273e0de10b0f208017e3e","target":"record","created_at":"2026-05-18T01:46:58Z","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":"245ec70bf82b2b9fbae369bfe564a34d4ca11018b6699e745c5c09d7ae28c068","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-17T07:50:43Z","title_canon_sha256":"3db149678fbc1475a9794e61e635c73a552a117c9d17faa08ad5387c4d733329"},"schema_version":"1.0","source":{"id":"1310.4604","kind":"arxiv","version":1}},"canonical_sha256":"551259fa1df73268a94bf1e827eef25b3e7644d615f475db86d6392a9a059661","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"551259fa1df73268a94bf1e827eef25b3e7644d615f475db86d6392a9a059661","first_computed_at":"2026-05-18T01:46:58.557534Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:46:58.557534Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jEni4Tho+d2Megi00xmy9i4f8hjFCli3n/qIqjOeLFA/5LZZdqEEFpOu7r57E8rg5VHSU6lPHWdBqB7ExuifBw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:46:58.558052Z","signed_message":"canonical_sha256_bytes"},"source_id":"1310.4604","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cd2919e91630034748cba77a7cd8ab67bd296924319273e0de10b0f208017e3e","sha256:b8c132ff0a4a6438452f3370ac9ba08ba030ce7ee55b3a41dc99cec9fea6308b"],"state_sha256":"186f578932a3c032798c5242ca2aa9091f807c8d47d29ac52ecf9f2d93b15a59"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AWGGzCU/U0lw25sKCrONcVYplYPxoxLq3e3Muzau0Vlr5Kf11j70jkWLi0zP7gb1NB/N1ir++xpctFmqWSRcBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T22:18:49.308541Z","bundle_sha256":"471bda0fa833ae9feacfae11718109a890c94756357293ff2e857b19c7e06d32"}}