{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:JFAIYXMGCJ5XM3B4KD7CWGH3DA","short_pith_number":"pith:JFAIYXMG","canonical_record":{"source":{"id":"1510.04308","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-10-14T20:47:24Z","cross_cats_sorted":["cond-mat.stat-mech","physics.comp-ph","quant-ph"],"title_canon_sha256":"8f8d95f421ea80256f625b75e3b7bb9fb1ecc93160c92860d52329c98ab73b04","abstract_canon_sha256":"f546b404d075f0ea1560948b5cdc5cf1ec1c16b5f40437cc77ec827813926668"},"schema_version":"1.0"},"canonical_sha256":"49408c5d86127b766c3c50fe2b18fb1800c0c73352fd93133d57403f70e0dc9f","source":{"kind":"arxiv","id":"1510.04308","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1510.04308","created_at":"2026-05-18T01:30:07Z"},{"alias_kind":"arxiv_version","alias_value":"1510.04308v1","created_at":"2026-05-18T01:30:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.04308","created_at":"2026-05-18T01:30:07Z"},{"alias_kind":"pith_short_12","alias_value":"JFAIYXMGCJ5X","created_at":"2026-05-18T12:29:27Z"},{"alias_kind":"pith_short_16","alias_value":"JFAIYXMGCJ5XM3B4","created_at":"2026-05-18T12:29:27Z"},{"alias_kind":"pith_short_8","alias_value":"JFAIYXMG","created_at":"2026-05-18T12:29:27Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:JFAIYXMGCJ5XM3B4KD7CWGH3DA","target":"record","payload":{"canonical_record":{"source":{"id":"1510.04308","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-10-14T20:47:24Z","cross_cats_sorted":["cond-mat.stat-mech","physics.comp-ph","quant-ph"],"title_canon_sha256":"8f8d95f421ea80256f625b75e3b7bb9fb1ecc93160c92860d52329c98ab73b04","abstract_canon_sha256":"f546b404d075f0ea1560948b5cdc5cf1ec1c16b5f40437cc77ec827813926668"},"schema_version":"1.0"},"canonical_sha256":"49408c5d86127b766c3c50fe2b18fb1800c0c73352fd93133d57403f70e0dc9f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:30:07.523394Z","signature_b64":"yIXjQ3NreSLdkyyYjZGVDbNBA3ohA3c/VCANi10LFwvWDsKLEe0AOfQ/JVoNpznVUi4nDbSUpQgaPc4Et2cVBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"49408c5d86127b766c3c50fe2b18fb1800c0c73352fd93133d57403f70e0dc9f","last_reissued_at":"2026-05-18T01:30:07.522605Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:30:07.522605Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1510.04308","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":"2026-05-18T01:30:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5xDT1KsHrl5nD1c3gjFJ6DB5X24uJis0MYJjCpyQzazae3BcIEzCqsZ90aUSihMeF1CEZEoaamf/kIOwnePkAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T19:57:36.468871Z"},"content_sha256":"b80dfd18f75474526f11efcda8291af3063821607a994433c7eb6cad0802a60a","schema_version":"1.0","event_id":"sha256:b80dfd18f75474526f11efcda8291af3063821607a994433c7eb6cad0802a60a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:JFAIYXMGCJ5XM3B4KD7CWGH3DA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Complex non-Hermitian Potentials and Real-Time Time-Dependent Density Functional Theory: A Master Equation Approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","physics.comp-ph","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Hanning Chen, Justin E. Elenewski, Yanxiang Zhao","submitted_at":"2015-10-14T20:47:24Z","abstract_excerpt":"The simulation of quantum transport in a realistic, many-particle system is a nontrivial problem with no quantitatively satisfactory solution. While real-time propagation has the potential to overcome the shortcomings of conventional transport methods, this approach is prone to finite size effects that are associated with modeling an open system on a closed spatial domain. Using a master equation framework, we exploit an equivalence between the superoperators coupling an open system to external particle reservoirs and non-Hermitian terms defined at the periphery of a quantum device. By taking "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.04308","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":"2026-05-18T01:30:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HawrzGkDiwD8WfqVtam4sn5XkpS/ZTh1cPfzHYD8otECXCe0P3FrXiOLQHrICwJVEZHhud1MMN0RK2pPub8FBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T19:57:36.469225Z"},"content_sha256":"d96003a1e397760b832c6fef73131fc45bf6f1f11f31ae3f274b25d162e72b54","schema_version":"1.0","event_id":"sha256:d96003a1e397760b832c6fef73131fc45bf6f1f11f31ae3f274b25d162e72b54"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JFAIYXMGCJ5XM3B4KD7CWGH3DA/bundle.json","state_url":"https://pith.science/pith/JFAIYXMGCJ5XM3B4KD7CWGH3DA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JFAIYXMGCJ5XM3B4KD7CWGH3DA/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":"2026-06-10T19:57:36Z","links":{"resolver":"https://pith.science/pith/JFAIYXMGCJ5XM3B4KD7CWGH3DA","bundle":"https://pith.science/pith/JFAIYXMGCJ5XM3B4KD7CWGH3DA/bundle.json","state":"https://pith.science/pith/JFAIYXMGCJ5XM3B4KD7CWGH3DA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JFAIYXMGCJ5XM3B4KD7CWGH3DA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:JFAIYXMGCJ5XM3B4KD7CWGH3DA","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":"f546b404d075f0ea1560948b5cdc5cf1ec1c16b5f40437cc77ec827813926668","cross_cats_sorted":["cond-mat.stat-mech","physics.comp-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-10-14T20:47:24Z","title_canon_sha256":"8f8d95f421ea80256f625b75e3b7bb9fb1ecc93160c92860d52329c98ab73b04"},"schema_version":"1.0","source":{"id":"1510.04308","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1510.04308","created_at":"2026-05-18T01:30:07Z"},{"alias_kind":"arxiv_version","alias_value":"1510.04308v1","created_at":"2026-05-18T01:30:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.04308","created_at":"2026-05-18T01:30:07Z"},{"alias_kind":"pith_short_12","alias_value":"JFAIYXMGCJ5X","created_at":"2026-05-18T12:29:27Z"},{"alias_kind":"pith_short_16","alias_value":"JFAIYXMGCJ5XM3B4","created_at":"2026-05-18T12:29:27Z"},{"alias_kind":"pith_short_8","alias_value":"JFAIYXMG","created_at":"2026-05-18T12:29:27Z"}],"graph_snapshots":[{"event_id":"sha256:d96003a1e397760b832c6fef73131fc45bf6f1f11f31ae3f274b25d162e72b54","target":"graph","created_at":"2026-05-18T01:30:07Z","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":"The simulation of quantum transport in a realistic, many-particle system is a nontrivial problem with no quantitatively satisfactory solution. While real-time propagation has the potential to overcome the shortcomings of conventional transport methods, this approach is prone to finite size effects that are associated with modeling an open system on a closed spatial domain. Using a master equation framework, we exploit an equivalence between the superoperators coupling an open system to external particle reservoirs and non-Hermitian terms defined at the periphery of a quantum device. By taking ","authors_text":"Hanning Chen, Justin E. Elenewski, Yanxiang Zhao","cross_cats":["cond-mat.stat-mech","physics.comp-ph","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-10-14T20:47:24Z","title":"Complex non-Hermitian Potentials and Real-Time Time-Dependent Density Functional Theory: A Master Equation Approach"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.04308","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:b80dfd18f75474526f11efcda8291af3063821607a994433c7eb6cad0802a60a","target":"record","created_at":"2026-05-18T01:30:07Z","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":"f546b404d075f0ea1560948b5cdc5cf1ec1c16b5f40437cc77ec827813926668","cross_cats_sorted":["cond-mat.stat-mech","physics.comp-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-10-14T20:47:24Z","title_canon_sha256":"8f8d95f421ea80256f625b75e3b7bb9fb1ecc93160c92860d52329c98ab73b04"},"schema_version":"1.0","source":{"id":"1510.04308","kind":"arxiv","version":1}},"canonical_sha256":"49408c5d86127b766c3c50fe2b18fb1800c0c73352fd93133d57403f70e0dc9f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"49408c5d86127b766c3c50fe2b18fb1800c0c73352fd93133d57403f70e0dc9f","first_computed_at":"2026-05-18T01:30:07.522605Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:30:07.522605Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yIXjQ3NreSLdkyyYjZGVDbNBA3ohA3c/VCANi10LFwvWDsKLEe0AOfQ/JVoNpznVUi4nDbSUpQgaPc4Et2cVBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:30:07.523394Z","signed_message":"canonical_sha256_bytes"},"source_id":"1510.04308","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b80dfd18f75474526f11efcda8291af3063821607a994433c7eb6cad0802a60a","sha256:d96003a1e397760b832c6fef73131fc45bf6f1f11f31ae3f274b25d162e72b54"],"state_sha256":"e2e40c9ec7f0382c2283d3c345e43a9f3709d13a936a346320271b619bbf8f31"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CkuGNITiaPHvmjAHtriWm1NFQPLqvF0Ea/0VAt0DaqDqV8iDczhsBEHx2Z2p2WZVm+5RWJ3vdm7x1ckyAjQZBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T19:57:36.471226Z","bundle_sha256":"0617ad124310f8cbfe0b840ba9922f6b880a73fa7d14ce19619d8796887804a3"}}