{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:6KDFL7RYCZZ227QPWJ5ZU26DRE","short_pith_number":"pith:6KDFL7RY","schema_version":"1.0","canonical_sha256":"f28655fe381673ad7e0fb27b9a6bc38936620665cab986f32ee85c7fd020cd08","source":{"kind":"arxiv","id":"1311.7394","version":2},"attestation_state":"computed","paper":{"title":"A generic map from non-Lindblad to Lindblad master equations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"quant-ph","authors_text":"Igor Lesanovsky, Juan P. Garrahan, Michael R. Hush","submitted_at":"2013-11-28T18:20:36Z","abstract_excerpt":"Many current problems of interest in quantum non-equilibrium are described by time-local master equations (TLMEs) for the density matrix that are not of the Lindblad form, that is, that are not strictly probability conserving and/or Markovian. Here we describe an generic approach by which the system of interest that obeys the TLME is coupled to an ancilla, such that the dynamics of the combined system-plus-ancilla is Markovian and thus described by a Lindblad equation. This in turn allows us to recover the properties of the original TLME dynamics from a physical unravelling of this associated "},"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":"1311.7394","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-11-28T18:20:36Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"fa3f3472aabe1ec30a3c520378ba7c6318a33c87375005d3517859e4d7568d10","abstract_canon_sha256":"196d7bfc158d66880c87ee89cf5db03d0269056c22fd2ad81fb7ec4365ab5e89"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:20:37.028941Z","signature_b64":"ISfWnWsonAhkW/XB/ZSWaXUugPKBtEUD+vEq0pRVu/tsaQLld3V+iTsHQKnYa/SAlvrcqnPU2Um4bJeMlBkWAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f28655fe381673ad7e0fb27b9a6bc38936620665cab986f32ee85c7fd020cd08","last_reissued_at":"2026-05-18T02:20:37.028233Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:20:37.028233Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A generic map from non-Lindblad to Lindblad master equations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"quant-ph","authors_text":"Igor Lesanovsky, Juan P. Garrahan, Michael R. Hush","submitted_at":"2013-11-28T18:20:36Z","abstract_excerpt":"Many current problems of interest in quantum non-equilibrium are described by time-local master equations (TLMEs) for the density matrix that are not of the Lindblad form, that is, that are not strictly probability conserving and/or Markovian. Here we describe an generic approach by which the system of interest that obeys the TLME is coupled to an ancilla, such that the dynamics of the combined system-plus-ancilla is Markovian and thus described by a Lindblad equation. This in turn allows us to recover the properties of the original TLME dynamics from a physical unravelling of this associated "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.7394","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":"1311.7394","created_at":"2026-05-18T02:20:37.028351+00:00"},{"alias_kind":"arxiv_version","alias_value":"1311.7394v2","created_at":"2026-05-18T02:20:37.028351+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.7394","created_at":"2026-05-18T02:20:37.028351+00:00"},{"alias_kind":"pith_short_12","alias_value":"6KDFL7RYCZZ2","created_at":"2026-05-18T12:27:36.564083+00:00"},{"alias_kind":"pith_short_16","alias_value":"6KDFL7RYCZZ227QP","created_at":"2026-05-18T12:27:36.564083+00:00"},{"alias_kind":"pith_short_8","alias_value":"6KDFL7RY","created_at":"2026-05-18T12:27:36.564083+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/6KDFL7RYCZZ227QPWJ5ZU26DRE","json":"https://pith.science/pith/6KDFL7RYCZZ227QPWJ5ZU26DRE.json","graph_json":"https://pith.science/api/pith-number/6KDFL7RYCZZ227QPWJ5ZU26DRE/graph.json","events_json":"https://pith.science/api/pith-number/6KDFL7RYCZZ227QPWJ5ZU26DRE/events.json","paper":"https://pith.science/paper/6KDFL7RY"},"agent_actions":{"view_html":"https://pith.science/pith/6KDFL7RYCZZ227QPWJ5ZU26DRE","download_json":"https://pith.science/pith/6KDFL7RYCZZ227QPWJ5ZU26DRE.json","view_paper":"https://pith.science/paper/6KDFL7RY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1311.7394&json=true","fetch_graph":"https://pith.science/api/pith-number/6KDFL7RYCZZ227QPWJ5ZU26DRE/graph.json","fetch_events":"https://pith.science/api/pith-number/6KDFL7RYCZZ227QPWJ5ZU26DRE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6KDFL7RYCZZ227QPWJ5ZU26DRE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6KDFL7RYCZZ227QPWJ5ZU26DRE/action/storage_attestation","attest_author":"https://pith.science/pith/6KDFL7RYCZZ227QPWJ5ZU26DRE/action/author_attestation","sign_citation":"https://pith.science/pith/6KDFL7RYCZZ227QPWJ5ZU26DRE/action/citation_signature","submit_replication":"https://pith.science/pith/6KDFL7RYCZZ227QPWJ5ZU26DRE/action/replication_record"}},"created_at":"2026-05-18T02:20:37.028351+00:00","updated_at":"2026-05-18T02:20:37.028351+00:00"}