{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:7SMFLCO5OW2P3UQ32KPMWBPYWS","short_pith_number":"pith:7SMFLCO5","schema_version":"1.0","canonical_sha256":"fc985589dd75b4fdd21bd29ecb05f8b4a613b0b3635caae4e05bcde4433c467e","source":{"kind":"arxiv","id":"1609.09636","version":1},"attestation_state":"computed","paper":{"title":"Stochastic pure state representation for open quantum systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Lajos Di\\'osi","submitted_at":"2016-09-30T08:51:27Z","abstract_excerpt":"We show that the usual master equation formalism of Markovian open quantum systems is completely equivalent to a certain state vector formalism. The state vector of the system satisfies a given frictional Schr\\\"odinger equation except for random instant transitions of discrete nature. Hasse's frictional Hamiltonian is recovered for the damped harmonic oscillator."},"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":"1609.09636","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-09-30T08:51:27Z","cross_cats_sorted":[],"title_canon_sha256":"4162e0bf9ed5c1b6e935c9f4f950c0244578466dca064fbfb6a046f998d9f9b7","abstract_canon_sha256":"820efd769368da256813a3221f35fb06cf4517ec14cd72c09024d49171101289"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:03:35.488445Z","signature_b64":"SpqmA3hRx2HCWkzkiPTj67QsV/Lg8Bvieb6F5z+v6sopfGBJruo2bXCAhRSpkUgl7cCdPgoX1hI0h+IyGW2HCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fc985589dd75b4fdd21bd29ecb05f8b4a613b0b3635caae4e05bcde4433c467e","last_reissued_at":"2026-05-18T01:03:35.487725Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:03:35.487725Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Stochastic pure state representation for open quantum systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Lajos Di\\'osi","submitted_at":"2016-09-30T08:51:27Z","abstract_excerpt":"We show that the usual master equation formalism of Markovian open quantum systems is completely equivalent to a certain state vector formalism. The state vector of the system satisfies a given frictional Schr\\\"odinger equation except for random instant transitions of discrete nature. Hasse's frictional Hamiltonian is recovered for the damped harmonic oscillator."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.09636","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1609.09636","created_at":"2026-05-18T01:03:35.487830+00:00"},{"alias_kind":"arxiv_version","alias_value":"1609.09636v1","created_at":"2026-05-18T01:03:35.487830+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.09636","created_at":"2026-05-18T01:03:35.487830+00:00"},{"alias_kind":"pith_short_12","alias_value":"7SMFLCO5OW2P","created_at":"2026-05-18T12:30:04.600751+00:00"},{"alias_kind":"pith_short_16","alias_value":"7SMFLCO5OW2P3UQ3","created_at":"2026-05-18T12:30:04.600751+00:00"},{"alias_kind":"pith_short_8","alias_value":"7SMFLCO5","created_at":"2026-05-18T12:30:04.600751+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/7SMFLCO5OW2P3UQ32KPMWBPYWS","json":"https://pith.science/pith/7SMFLCO5OW2P3UQ32KPMWBPYWS.json","graph_json":"https://pith.science/api/pith-number/7SMFLCO5OW2P3UQ32KPMWBPYWS/graph.json","events_json":"https://pith.science/api/pith-number/7SMFLCO5OW2P3UQ32KPMWBPYWS/events.json","paper":"https://pith.science/paper/7SMFLCO5"},"agent_actions":{"view_html":"https://pith.science/pith/7SMFLCO5OW2P3UQ32KPMWBPYWS","download_json":"https://pith.science/pith/7SMFLCO5OW2P3UQ32KPMWBPYWS.json","view_paper":"https://pith.science/paper/7SMFLCO5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1609.09636&json=true","fetch_graph":"https://pith.science/api/pith-number/7SMFLCO5OW2P3UQ32KPMWBPYWS/graph.json","fetch_events":"https://pith.science/api/pith-number/7SMFLCO5OW2P3UQ32KPMWBPYWS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7SMFLCO5OW2P3UQ32KPMWBPYWS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7SMFLCO5OW2P3UQ32KPMWBPYWS/action/storage_attestation","attest_author":"https://pith.science/pith/7SMFLCO5OW2P3UQ32KPMWBPYWS/action/author_attestation","sign_citation":"https://pith.science/pith/7SMFLCO5OW2P3UQ32KPMWBPYWS/action/citation_signature","submit_replication":"https://pith.science/pith/7SMFLCO5OW2P3UQ32KPMWBPYWS/action/replication_record"}},"created_at":"2026-05-18T01:03:35.487830+00:00","updated_at":"2026-05-18T01:03:35.487830+00:00"}