{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:VNFEIFWMA2JDWP4ZI7DKMGKDZU","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":"e080c9c056f9f5c420d8629a7775901074d70a9d7377237c563ed63cf12eb814","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-11-20T10:10:28Z","title_canon_sha256":"a6824c1b8234929d2d00dece4c949bd397bc0543aac723b0980136fb6a015ea3"},"schema_version":"1.0","source":{"id":"1811.08161","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1811.08161","created_at":"2026-05-18T00:00:13Z"},{"alias_kind":"arxiv_version","alias_value":"1811.08161v1","created_at":"2026-05-18T00:00:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.08161","created_at":"2026-05-18T00:00:13Z"},{"alias_kind":"pith_short_12","alias_value":"VNFEIFWMA2JD","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_16","alias_value":"VNFEIFWMA2JDWP4Z","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_8","alias_value":"VNFEIFWM","created_at":"2026-05-18T12:32:59Z"}],"graph_snapshots":[{"event_id":"sha256:69ff03e4d488585c24c5ef52428477f6974c6b6db93f2177eb6b259154aba8a4","target":"graph","created_at":"2026-05-18T00:00:13Z","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":"Modeling many-body quantum systems with strong interactions is one of the core challenges of modern physics. A range of methods has been developed to approach this task, each with its own idiosyncrasies, approximations, and realm of applicability. Perhaps the most successful and ubiquitous of these approaches is density functional theory (DFT). Its Kohn-Sham formulation has been the basis for many fundamental physical insights, and it has been successfully applied to fields as diverse as quantum chemistry, condensed matter and dense plasmas. Despite the progress made by DFT and related schemes","authors_text":"Brett Larder, Dirk Gericke, Gianluca Gregori, Paul Mabey, Scott Richardson, Thomas White","cross_cats":["physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-11-20T10:10:28Z","title":"Fast Non-Adiabatic Dynamics of Many-Body Quantum Systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.08161","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":"sha256:32e1fa8fc3ec35f0a57a5bce1490ff549348ba8438c8034f14b1ad3aabe0cb37","target":"record","created_at":"2026-05-18T00:00:13Z","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":"e080c9c056f9f5c420d8629a7775901074d70a9d7377237c563ed63cf12eb814","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-11-20T10:10:28Z","title_canon_sha256":"a6824c1b8234929d2d00dece4c949bd397bc0543aac723b0980136fb6a015ea3"},"schema_version":"1.0","source":{"id":"1811.08161","kind":"arxiv","version":1}},"canonical_sha256":"ab4a4416cc06923b3f9947c6a61943cd16fd6455346bbc0e451ee3b70a5e57d2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ab4a4416cc06923b3f9947c6a61943cd16fd6455346bbc0e451ee3b70a5e57d2","first_computed_at":"2026-05-18T00:00:13.985034Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:00:13.985034Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"b/WRH/kVYCdXcjKJdT1iOmgtu0Dx8nG9T7J2SAtYXT2EU/wqdDwshcQmFVsx6kiX5EFXCXvCQUxb66s+CJeWCA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:00:13.985566Z","signed_message":"canonical_sha256_bytes"},"source_id":"1811.08161","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:32e1fa8fc3ec35f0a57a5bce1490ff549348ba8438c8034f14b1ad3aabe0cb37","sha256:69ff03e4d488585c24c5ef52428477f6974c6b6db93f2177eb6b259154aba8a4"],"state_sha256":"f8470d4ae95bd5ef6c4f2fad8c631556fd65cc5415d320fe1f135698317463df"}