{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:K4MCM5F4L4G45LHDWBVDV5SUK6","short_pith_number":"pith:K4MCM5F4","canonical_record":{"source":{"id":"1604.01082","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-04-04T22:43:26Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con","quant-ph"],"title_canon_sha256":"79508db8477747bd441d6d74fbdd5dc7a9fb0cd20e2ef18778176f052b0e49b2","abstract_canon_sha256":"15e36a848ece570f83cd05b85c0ece03316eeacacd196430b611a68b317ccd69"},"schema_version":"1.0"},"canonical_sha256":"57182674bc5f0dceace3b06a3af65457818f8ba96f3ea0444f906eda7d41ddcd","source":{"kind":"arxiv","id":"1604.01082","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.01082","created_at":"2026-05-18T00:51:51Z"},{"alias_kind":"arxiv_version","alias_value":"1604.01082v3","created_at":"2026-05-18T00:51:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.01082","created_at":"2026-05-18T00:51:51Z"},{"alias_kind":"pith_short_12","alias_value":"K4MCM5F4L4G4","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_16","alias_value":"K4MCM5F4L4G45LHD","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_8","alias_value":"K4MCM5F4","created_at":"2026-05-18T12:30:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:K4MCM5F4L4G45LHDWBVDV5SUK6","target":"record","payload":{"canonical_record":{"source":{"id":"1604.01082","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-04-04T22:43:26Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con","quant-ph"],"title_canon_sha256":"79508db8477747bd441d6d74fbdd5dc7a9fb0cd20e2ef18778176f052b0e49b2","abstract_canon_sha256":"15e36a848ece570f83cd05b85c0ece03316eeacacd196430b611a68b317ccd69"},"schema_version":"1.0"},"canonical_sha256":"57182674bc5f0dceace3b06a3af65457818f8ba96f3ea0444f906eda7d41ddcd","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:51:51.462181Z","signature_b64":"3ijgcFGEDeHA6FJ0kZ4QgdzY6gBupb+38xfWyWz70ii2ueEcfUncTIginAYtTonfzkbYHQNt/jTnz8vQQUabBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"57182674bc5f0dceace3b06a3af65457818f8ba96f3ea0444f906eda7d41ddcd","last_reissued_at":"2026-05-18T00:51:51.461493Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:51:51.461493Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1604.01082","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:51:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3asFuRxxR3Hd2nmBkKbEOdFhoRoSolnk4z77/6REMhv4DDjqF1DOZilAhcFPB9Bw9mJMpwBrwaVVr8dZWX6ZBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T21:39:12.122627Z"},"content_sha256":"b94ab695bdd5d33448e69da73d0eae39bd6e5d90319a290b1533c0206370531f","schema_version":"1.0","event_id":"sha256:b94ab695bdd5d33448e69da73d0eae39bd6e5d90319a290b1533c0206370531f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:K4MCM5F4L4G45LHDWBVDV5SUK6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Markovian Quantum Master Equation beyond Adiabatic Regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.supr-con","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Makoto Yamaguchi, Tatsuro Yuge, Tetsuo Ogawa","submitted_at":"2016-04-04T22:43:26Z","abstract_excerpt":"By introducing a temporal change timescale $\\tau_{\\text{A}}(t)$ for the time-dependent system Hamiltonian, a general formulation of the Markovian quantum master equation is given to go well beyond the adiabatic regime. In appropriate situations, the framework is well justified even if $\\tau_{\\text{A}}(t)$ is faster than the decay timescale of the bath correlation function. An application to the dissipative Landau-Zener model demonstrates this general result. The findings are applicable to a wide range of fields, providing a basis for quantum control beyond the adiabatic regime."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.01082","kind":"arxiv","version":3},"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":"2026-05-18T00:51:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pBpw/RzW3qGS+oqaXtF+ZmhaTchneBEtlv1xytIe4psAh741Uj2/4aDepOBhtmAfooZol+3eKi3V84ONnNVnDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T21:39:12.123329Z"},"content_sha256":"48a7aa4a407786b447998fca68e11fb947a1392d16bae93298d1052eba9d1492","schema_version":"1.0","event_id":"sha256:48a7aa4a407786b447998fca68e11fb947a1392d16bae93298d1052eba9d1492"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/K4MCM5F4L4G45LHDWBVDV5SUK6/bundle.json","state_url":"https://pith.science/pith/K4MCM5F4L4G45LHDWBVDV5SUK6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/K4MCM5F4L4G45LHDWBVDV5SUK6/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":"2026-05-27T21:39:12Z","links":{"resolver":"https://pith.science/pith/K4MCM5F4L4G45LHDWBVDV5SUK6","bundle":"https://pith.science/pith/K4MCM5F4L4G45LHDWBVDV5SUK6/bundle.json","state":"https://pith.science/pith/K4MCM5F4L4G45LHDWBVDV5SUK6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/K4MCM5F4L4G45LHDWBVDV5SUK6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:K4MCM5F4L4G45LHDWBVDV5SUK6","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":"15e36a848ece570f83cd05b85c0ece03316eeacacd196430b611a68b317ccd69","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-04-04T22:43:26Z","title_canon_sha256":"79508db8477747bd441d6d74fbdd5dc7a9fb0cd20e2ef18778176f052b0e49b2"},"schema_version":"1.0","source":{"id":"1604.01082","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.01082","created_at":"2026-05-18T00:51:51Z"},{"alias_kind":"arxiv_version","alias_value":"1604.01082v3","created_at":"2026-05-18T00:51:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.01082","created_at":"2026-05-18T00:51:51Z"},{"alias_kind":"pith_short_12","alias_value":"K4MCM5F4L4G4","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_16","alias_value":"K4MCM5F4L4G45LHD","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_8","alias_value":"K4MCM5F4","created_at":"2026-05-18T12:30:25Z"}],"graph_snapshots":[{"event_id":"sha256:48a7aa4a407786b447998fca68e11fb947a1392d16bae93298d1052eba9d1492","target":"graph","created_at":"2026-05-18T00:51:51Z","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":"By introducing a temporal change timescale $\\tau_{\\text{A}}(t)$ for the time-dependent system Hamiltonian, a general formulation of the Markovian quantum master equation is given to go well beyond the adiabatic regime. In appropriate situations, the framework is well justified even if $\\tau_{\\text{A}}(t)$ is faster than the decay timescale of the bath correlation function. An application to the dissipative Landau-Zener model demonstrates this general result. The findings are applicable to a wide range of fields, providing a basis for quantum control beyond the adiabatic regime.","authors_text":"Makoto Yamaguchi, Tatsuro Yuge, Tetsuo Ogawa","cross_cats":["cond-mat.mes-hall","cond-mat.supr-con","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-04-04T22:43:26Z","title":"Markovian Quantum Master Equation beyond Adiabatic Regime"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.01082","kind":"arxiv","version":3},"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:b94ab695bdd5d33448e69da73d0eae39bd6e5d90319a290b1533c0206370531f","target":"record","created_at":"2026-05-18T00:51:51Z","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":"15e36a848ece570f83cd05b85c0ece03316eeacacd196430b611a68b317ccd69","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2016-04-04T22:43:26Z","title_canon_sha256":"79508db8477747bd441d6d74fbdd5dc7a9fb0cd20e2ef18778176f052b0e49b2"},"schema_version":"1.0","source":{"id":"1604.01082","kind":"arxiv","version":3}},"canonical_sha256":"57182674bc5f0dceace3b06a3af65457818f8ba96f3ea0444f906eda7d41ddcd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"57182674bc5f0dceace3b06a3af65457818f8ba96f3ea0444f906eda7d41ddcd","first_computed_at":"2026-05-18T00:51:51.461493Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:51:51.461493Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"3ijgcFGEDeHA6FJ0kZ4QgdzY6gBupb+38xfWyWz70ii2ueEcfUncTIginAYtTonfzkbYHQNt/jTnz8vQQUabBg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:51:51.462181Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.01082","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b94ab695bdd5d33448e69da73d0eae39bd6e5d90319a290b1533c0206370531f","sha256:48a7aa4a407786b447998fca68e11fb947a1392d16bae93298d1052eba9d1492"],"state_sha256":"04f4e5983352829eba15d7520c2933f80794886183530a393d9cda58908a1c72"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0f3TG16zyLuRRZsoGqqjVHQca/+t4u3Jzrii/TXON//sL0/o9sTs9gg9eb8yMr99VcqEWc5MlAwu4oBz3D5nAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T21:39:12.126899Z","bundle_sha256":"fbcc88932da313aeb73cfbcfa66e509913ffb3701063971c4d02e8d40d3b37c9"}}