{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:IAOSCFRFJQZH43B6KUWBVVDASK","short_pith_number":"pith:IAOSCFRF","canonical_record":{"source":{"id":"1712.06397","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-12-18T13:45:55Z","cross_cats_sorted":[],"title_canon_sha256":"b4bcb17196005daec606c3dfde5728e2dd9b3bf5584f8454c4cc4982e52d1a38","abstract_canon_sha256":"b8f41c9d9130b852b2dfd7e4ea73aa677ab6995216b17d673610e40f786a6634"},"schema_version":"1.0"},"canonical_sha256":"401d2116254c327e6c3e552c1ad460929147df5a3e4c15ea4c69b310d85def46","source":{"kind":"arxiv","id":"1712.06397","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1712.06397","created_at":"2026-05-18T00:11:39Z"},{"alias_kind":"arxiv_version","alias_value":"1712.06397v1","created_at":"2026-05-18T00:11:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.06397","created_at":"2026-05-18T00:11:39Z"},{"alias_kind":"pith_short_12","alias_value":"IAOSCFRFJQZH","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"IAOSCFRFJQZH43B6","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"IAOSCFRF","created_at":"2026-05-18T12:31:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:IAOSCFRFJQZH43B6KUWBVVDASK","target":"record","payload":{"canonical_record":{"source":{"id":"1712.06397","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-12-18T13:45:55Z","cross_cats_sorted":[],"title_canon_sha256":"b4bcb17196005daec606c3dfde5728e2dd9b3bf5584f8454c4cc4982e52d1a38","abstract_canon_sha256":"b8f41c9d9130b852b2dfd7e4ea73aa677ab6995216b17d673610e40f786a6634"},"schema_version":"1.0"},"canonical_sha256":"401d2116254c327e6c3e552c1ad460929147df5a3e4c15ea4c69b310d85def46","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:11:39.458437Z","signature_b64":"IQKbw+3+ZwVR5NMw/nJkCV60oSNQ+K3oBRBmVfuPxbngCWHBoEjrJeMpks/Jp73al6l0HEnksl2zQIpNKT9+Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"401d2116254c327e6c3e552c1ad460929147df5a3e4c15ea4c69b310d85def46","last_reissued_at":"2026-05-18T00:11:39.457730Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:11:39.457730Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1712.06397","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":"2026-05-18T00:11:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XVU3VEJ3cDoMaJvAEFL5LiQieT3Sj+n8dz+VK3Webi4yP+4WnKfWHwBQIhkgSIsQQgt4gmctSKHmr4UshJatDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-01T17:18:54.410273Z"},"content_sha256":"e53f78442de48dba7ecc0ce1294844847ae1ec50d844c2acd51d019b6f6bb707","schema_version":"1.0","event_id":"sha256:e53f78442de48dba7ecc0ce1294844847ae1ec50d844c2acd51d019b6f6bb707"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:IAOSCFRFJQZH43B6KUWBVVDASK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Driving Spin-Boson Models From Equilibrium Using Exact Quantum Dynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"C.D. Lorenz, G.M.G. McCaul, L. Kantorovich","submitted_at":"2017-12-18T13:45:55Z","abstract_excerpt":"We present an application of the Extended Stochastic Liouville Equation (ESLE) Phys. Rev. B 95, 125124, which gives an exact solution for the reduced density matrix of an open system surrounded by a harmonic heat bath. This method considers the extended system (the open system and the bath) being thermally equilibrated prior to the action of a time dependent perturbation, as opposed to the usual assumption that system and bath are initially partitioned. This is an exact technique capable of accounting for arbitrary parameter regimes of the model. Here we present our first numerical implementat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.06397","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":"2026-05-18T00:11:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ryj5nRgFMNWJ95xQsuNvfTMo9f7+mAzkvgkl66mrlF+L+6jbM5pt20Wo6uOH1M3BGZ2kKlK6o4lexLiiIkUdCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-01T17:18:54.410638Z"},"content_sha256":"be351091d0c0cde26dd2898a5b17385e88e309ff7d9c72cfd2b2b9a5bc88dc50","schema_version":"1.0","event_id":"sha256:be351091d0c0cde26dd2898a5b17385e88e309ff7d9c72cfd2b2b9a5bc88dc50"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IAOSCFRFJQZH43B6KUWBVVDASK/bundle.json","state_url":"https://pith.science/pith/IAOSCFRFJQZH43B6KUWBVVDASK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IAOSCFRFJQZH43B6KUWBVVDASK/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":"2026-07-01T17:18:54Z","links":{"resolver":"https://pith.science/pith/IAOSCFRFJQZH43B6KUWBVVDASK","bundle":"https://pith.science/pith/IAOSCFRFJQZH43B6KUWBVVDASK/bundle.json","state":"https://pith.science/pith/IAOSCFRFJQZH43B6KUWBVVDASK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IAOSCFRFJQZH43B6KUWBVVDASK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:IAOSCFRFJQZH43B6KUWBVVDASK","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":"b8f41c9d9130b852b2dfd7e4ea73aa677ab6995216b17d673610e40f786a6634","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-12-18T13:45:55Z","title_canon_sha256":"b4bcb17196005daec606c3dfde5728e2dd9b3bf5584f8454c4cc4982e52d1a38"},"schema_version":"1.0","source":{"id":"1712.06397","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1712.06397","created_at":"2026-05-18T00:11:39Z"},{"alias_kind":"arxiv_version","alias_value":"1712.06397v1","created_at":"2026-05-18T00:11:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.06397","created_at":"2026-05-18T00:11:39Z"},{"alias_kind":"pith_short_12","alias_value":"IAOSCFRFJQZH","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"IAOSCFRFJQZH43B6","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"IAOSCFRF","created_at":"2026-05-18T12:31:21Z"}],"graph_snapshots":[{"event_id":"sha256:be351091d0c0cde26dd2898a5b17385e88e309ff7d9c72cfd2b2b9a5bc88dc50","target":"graph","created_at":"2026-05-18T00:11:39Z","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 present an application of the Extended Stochastic Liouville Equation (ESLE) Phys. Rev. B 95, 125124, which gives an exact solution for the reduced density matrix of an open system surrounded by a harmonic heat bath. This method considers the extended system (the open system and the bath) being thermally equilibrated prior to the action of a time dependent perturbation, as opposed to the usual assumption that system and bath are initially partitioned. This is an exact technique capable of accounting for arbitrary parameter regimes of the model. Here we present our first numerical implementat","authors_text":"C.D. Lorenz, G.M.G. McCaul, L. Kantorovich","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-12-18T13:45:55Z","title":"Driving Spin-Boson Models From Equilibrium Using Exact Quantum Dynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.06397","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:e53f78442de48dba7ecc0ce1294844847ae1ec50d844c2acd51d019b6f6bb707","target":"record","created_at":"2026-05-18T00:11:39Z","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":"b8f41c9d9130b852b2dfd7e4ea73aa677ab6995216b17d673610e40f786a6634","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-12-18T13:45:55Z","title_canon_sha256":"b4bcb17196005daec606c3dfde5728e2dd9b3bf5584f8454c4cc4982e52d1a38"},"schema_version":"1.0","source":{"id":"1712.06397","kind":"arxiv","version":1}},"canonical_sha256":"401d2116254c327e6c3e552c1ad460929147df5a3e4c15ea4c69b310d85def46","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"401d2116254c327e6c3e552c1ad460929147df5a3e4c15ea4c69b310d85def46","first_computed_at":"2026-05-18T00:11:39.457730Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:11:39.457730Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IQKbw+3+ZwVR5NMw/nJkCV60oSNQ+K3oBRBmVfuPxbngCWHBoEjrJeMpks/Jp73al6l0HEnksl2zQIpNKT9+Cw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:11:39.458437Z","signed_message":"canonical_sha256_bytes"},"source_id":"1712.06397","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e53f78442de48dba7ecc0ce1294844847ae1ec50d844c2acd51d019b6f6bb707","sha256:be351091d0c0cde26dd2898a5b17385e88e309ff7d9c72cfd2b2b9a5bc88dc50"],"state_sha256":"d81ecd4777fe79c99fb38ef85773e205b615cdf59ab1590c3c7d30e0474fa934"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1C/wqdzGzhSKQH1ZZ1rpaFlJTUqst5fG7Eb8BJZ/ZReNtDgU9JcWlrLzJVXjrMZyamgVVueByZ9DSXAnt3ouCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-01T17:18:54.412617Z","bundle_sha256":"220ea47d247061a3eaeb91a07530c22013909b40d00737fd213dde022e64aad2"}}