{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:RUMZPN35QKSDOJW2Q3FKC3EFL3","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":"0b5b0f76040aacf253dcd224612633e092c51c86c2161bfa8056ab7c59c23dea","cross_cats_sorted":["cond-mat.mtrl-sci","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2012-12-11T12:55:22Z","title_canon_sha256":"af752a9119bd4aab8e250116e27c08d57c6c236240598ab6eb3efd17e5ff079d"},"schema_version":"1.0","source":{"id":"1212.2407","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.2407","created_at":"2026-05-18T01:52:40Z"},{"alias_kind":"arxiv_version","alias_value":"1212.2407v1","created_at":"2026-05-18T01:52:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.2407","created_at":"2026-05-18T01:52:40Z"},{"alias_kind":"pith_short_12","alias_value":"RUMZPN35QKSD","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"RUMZPN35QKSDOJW2","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"RUMZPN35","created_at":"2026-05-18T12:27:20Z"}],"graph_snapshots":[{"event_id":"sha256:3d57ae1a93cb6a8782b9891927f47814ca3d7677eb388462e7ec5ef7d373e8e2","target":"graph","created_at":"2026-05-18T01:52:40Z","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 apply the recently proposed quasi-classical approach for a second quantized many-electron Hamiltonian in Cartesian coordinates [J. Chem. Phys. 137, 154107 (2012)] to correlated nonequilibrium quantum transport. The approach provides accurate results for the resonant level model for a wide range of temperatures, bias and gate voltages, correcting for the flaws of our recently proposed mapping using action-angle variables. When electron-electron interactions are included, higher order schemes are required to map the two-electron integrals, leading to semi-quantitative results for the Anderson","authors_text":"Bin Li, David W.H. Swenson, Eran Rabani, Tal J. Levy, William H. Miller","cross_cats":["cond-mat.mtrl-sci","physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2012-12-11T12:55:22Z","title":"A Cartesian Quasi-classical Model to Nonequilibrium Quantum Transport: The Anderson Impurity Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.2407","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":"sha256:23b0618a051cb23fefc0af5963b1ab56a683228a7c9c10645c0136dc2a8a2ec9","target":"record","created_at":"2026-05-18T01:52:40Z","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":"0b5b0f76040aacf253dcd224612633e092c51c86c2161bfa8056ab7c59c23dea","cross_cats_sorted":["cond-mat.mtrl-sci","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2012-12-11T12:55:22Z","title_canon_sha256":"af752a9119bd4aab8e250116e27c08d57c6c236240598ab6eb3efd17e5ff079d"},"schema_version":"1.0","source":{"id":"1212.2407","kind":"arxiv","version":1}},"canonical_sha256":"8d1997b77d82a43726da86caa16c855efd70fc296d5b3ac11f94c5c652b3c9ea","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8d1997b77d82a43726da86caa16c855efd70fc296d5b3ac11f94c5c652b3c9ea","first_computed_at":"2026-05-18T01:52:40.091845Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:52:40.091845Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wPz2jcriGlqwjQX4F4fzzoIo+y2/+xR85tB9q0H3KkKgy9bSe91A97jNcpXzo8fZoXLwTGOYEngSoQc6HAEXAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:52:40.092582Z","signed_message":"canonical_sha256_bytes"},"source_id":"1212.2407","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:23b0618a051cb23fefc0af5963b1ab56a683228a7c9c10645c0136dc2a8a2ec9","sha256:3d57ae1a93cb6a8782b9891927f47814ca3d7677eb388462e7ec5ef7d373e8e2"],"state_sha256":"1c025652e6fdc1a05f8a58605f13694da1ee90aa692359e1ece9e1eee1c6e456"}