{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:SGLIPLG5MLOSXYE5YCTUUYPSRE","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":"2d01e53b41436c9a8bbb2609feaacec6fc087e7a01f9948e8735b1ddec4da65e","cross_cats_sorted":["cond-mat.mes-hall","physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-09-06T09:20:08Z","title_canon_sha256":"f42e95d8616d49ee7bc03185e799bc79f4cd799ff2f68e2c3cc68f4c0ebe1ac3"},"schema_version":"1.0","source":{"id":"2409.04145","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2409.04145","created_at":"2026-07-05T11:06:23Z"},{"alias_kind":"arxiv_version","alias_value":"2409.04145v2","created_at":"2026-07-05T11:06:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.04145","created_at":"2026-07-05T11:06:23Z"},{"alias_kind":"pith_short_12","alias_value":"SGLIPLG5MLOS","created_at":"2026-07-05T11:06:23Z"},{"alias_kind":"pith_short_16","alias_value":"SGLIPLG5MLOSXYE5","created_at":"2026-07-05T11:06:23Z"},{"alias_kind":"pith_short_8","alias_value":"SGLIPLG5","created_at":"2026-07-05T11:06:23Z"}],"graph_snapshots":[{"event_id":"sha256:15366ce7da07e8bcbf4f4dee103251ac51db760cc9348e51e122cd7781c29dd0","target":"graph","created_at":"2026-07-05T11:06:23Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2409.04145/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Being able to study the dynamics of quantum systems interacting with several environments is important in many settings ranging from quantum chemistry to quantum thermodynamics, through out-of-equilibrium systems. For such problems tensor network-based methods are state-of-the-art approaches for performing numerically exact simulations. However, to be used efficiently in this multi-environment and non-perturbative context, these methods require an optimized choice of the topology of the wave-function Ans\\\"atze. This is often done by analysing cross-correlations between different system and env","authors_text":"Alex W. Chin, Brendon W. Lovett, Thibaut Lacroix","cross_cats":["cond-mat.mes-hall","physics.comp-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-09-06T09:20:08Z","title":"Connectivity matters: Impact of bath modes ordering and geometry in open quantum system simulation with Tensor Network States"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.04145","kind":"arxiv","version":2},"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":"sha256:2e562cbceb541c7900c5c105c7ee7b81ee723743d65dab08315a3f98dc5c101e","target":"record","created_at":"2026-07-05T11:06:23Z","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":"2d01e53b41436c9a8bbb2609feaacec6fc087e7a01f9948e8735b1ddec4da65e","cross_cats_sorted":["cond-mat.mes-hall","physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-09-06T09:20:08Z","title_canon_sha256":"f42e95d8616d49ee7bc03185e799bc79f4cd799ff2f68e2c3cc68f4c0ebe1ac3"},"schema_version":"1.0","source":{"id":"2409.04145","kind":"arxiv","version":2}},"canonical_sha256":"919687acdd62dd2be09dc0a74a61f2892b1f14d56a56846cf170b98967e83909","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"919687acdd62dd2be09dc0a74a61f2892b1f14d56a56846cf170b98967e83909","first_computed_at":"2026-07-05T11:06:23.145019Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:06:23.145019Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"r6JgT5dIBNIawAKaHtwoFk+gpLNIiW4TMbPY6P9Tc0O4GmSRxvP9hDwl3/AnGm4oN/h0ya0N463INvHlLnO3Cg==","signature_status":"signed_v1","signed_at":"2026-07-05T11:06:23.145603Z","signed_message":"canonical_sha256_bytes"},"source_id":"2409.04145","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2e562cbceb541c7900c5c105c7ee7b81ee723743d65dab08315a3f98dc5c101e","sha256:15366ce7da07e8bcbf4f4dee103251ac51db760cc9348e51e122cd7781c29dd0"],"state_sha256":"3d0385652e4092799a060add4339597887ade4367c4cab1637a61f25e2c3fb08"}