{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:UITOKM54SY73V7ME2P3IHNGZEP","short_pith_number":"pith:UITOKM54","schema_version":"1.0","canonical_sha256":"a226e533bc963fbafd84d3f683b4d923d258266e4cb2f359a4940db72d3aba1f","source":{"kind":"arxiv","id":"1703.10775","version":2},"attestation_state":"computed","paper":{"title":"Dark state with counter-rotating dissipative channels","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"J. Q. You, Lian-Ao Wu, Mi Chen, Ting Yu, Zheng-Yang Zhou","submitted_at":"2017-03-31T07:21:51Z","abstract_excerpt":"Dark state as a consequence of interference between different quantum states has great importance in the fields of chip-scale atomic clock and quantum information. For the $\\Lambda$-type three-level system, this dark state is generally regarded as being dissipation-free because it is a superposition of two lowest states without dipole transition between them. However, previous studies are based on the rotating-wave approximation (RWA) by neglecting the counter-rotating terms in the system-environment interaction. In this work, we study non-Markovian quantum dynamics of the dark state in a $\\La"},"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":"1703.10775","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-03-31T07:21:51Z","cross_cats_sorted":[],"title_canon_sha256":"2f134cf65e3538fcb6b733dd323d132fea0bcac0a4d933bda1e7d113f13eb999","abstract_canon_sha256":"8f4033de1ced7a962cf302798d86916341077651071015983d6d73c8ec14a81f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:32:11.049578Z","signature_b64":"PDYWtVpTPU0H+++aFTgnojSfY8EplQZNs/AgxBiL5fOkQVDcmpE6NwsCgJyu2eDTa4LXSdGxrBD6fOqfUEeRAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a226e533bc963fbafd84d3f683b4d923d258266e4cb2f359a4940db72d3aba1f","last_reissued_at":"2026-05-18T00:32:11.048830Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:32:11.048830Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dark state with counter-rotating dissipative channels","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"J. Q. You, Lian-Ao Wu, Mi Chen, Ting Yu, Zheng-Yang Zhou","submitted_at":"2017-03-31T07:21:51Z","abstract_excerpt":"Dark state as a consequence of interference between different quantum states has great importance in the fields of chip-scale atomic clock and quantum information. For the $\\Lambda$-type three-level system, this dark state is generally regarded as being dissipation-free because it is a superposition of two lowest states without dipole transition between them. However, previous studies are based on the rotating-wave approximation (RWA) by neglecting the counter-rotating terms in the system-environment interaction. In this work, we study non-Markovian quantum dynamics of the dark state in a $\\La"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.10775","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":""},"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":"1703.10775","created_at":"2026-05-18T00:32:11.048951+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.10775v2","created_at":"2026-05-18T00:32:11.048951+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.10775","created_at":"2026-05-18T00:32:11.048951+00:00"},{"alias_kind":"pith_short_12","alias_value":"UITOKM54SY73","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_16","alias_value":"UITOKM54SY73V7ME","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_8","alias_value":"UITOKM54","created_at":"2026-05-18T12:31:46.661854+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/UITOKM54SY73V7ME2P3IHNGZEP","json":"https://pith.science/pith/UITOKM54SY73V7ME2P3IHNGZEP.json","graph_json":"https://pith.science/api/pith-number/UITOKM54SY73V7ME2P3IHNGZEP/graph.json","events_json":"https://pith.science/api/pith-number/UITOKM54SY73V7ME2P3IHNGZEP/events.json","paper":"https://pith.science/paper/UITOKM54"},"agent_actions":{"view_html":"https://pith.science/pith/UITOKM54SY73V7ME2P3IHNGZEP","download_json":"https://pith.science/pith/UITOKM54SY73V7ME2P3IHNGZEP.json","view_paper":"https://pith.science/paper/UITOKM54","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.10775&json=true","fetch_graph":"https://pith.science/api/pith-number/UITOKM54SY73V7ME2P3IHNGZEP/graph.json","fetch_events":"https://pith.science/api/pith-number/UITOKM54SY73V7ME2P3IHNGZEP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UITOKM54SY73V7ME2P3IHNGZEP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UITOKM54SY73V7ME2P3IHNGZEP/action/storage_attestation","attest_author":"https://pith.science/pith/UITOKM54SY73V7ME2P3IHNGZEP/action/author_attestation","sign_citation":"https://pith.science/pith/UITOKM54SY73V7ME2P3IHNGZEP/action/citation_signature","submit_replication":"https://pith.science/pith/UITOKM54SY73V7ME2P3IHNGZEP/action/replication_record"}},"created_at":"2026-05-18T00:32:11.048951+00:00","updated_at":"2026-05-18T00:32:11.048951+00:00"}