{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:WYXUV62NBSLLSELIQ7UH7335QA","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":"9f77d6145cc3e117e1538adb958816fed4cef26bd3b8576f50dbdaa2f3fa6554","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-08-18T15:40:46Z","title_canon_sha256":"deaefc621df1b55f5b05e590c3670834110ee8e9f2eeb9e4ea9cc451b93e2075"},"schema_version":"1.0","source":{"id":"2208.08917","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2208.08917","created_at":"2026-07-05T04:49:39Z"},{"alias_kind":"arxiv_version","alias_value":"2208.08917v1","created_at":"2026-07-05T04:49:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2208.08917","created_at":"2026-07-05T04:49:39Z"},{"alias_kind":"pith_short_12","alias_value":"WYXUV62NBSLL","created_at":"2026-07-05T04:49:39Z"},{"alias_kind":"pith_short_16","alias_value":"WYXUV62NBSLLSELI","created_at":"2026-07-05T04:49:39Z"},{"alias_kind":"pith_short_8","alias_value":"WYXUV62N","created_at":"2026-07-05T04:49:39Z"}],"graph_snapshots":[{"event_id":"sha256:2845876548a432deb0a10853ff4ae5f5e29c081994cc2baf1f1c5a20f590ad9d","target":"graph","created_at":"2026-07-05T04:49:39Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2208.08917/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present a new quantum molecular dynamics (MD) method where the electronic structure and atomic forces are solved by a real-space dynamical mean-field theory (DMFT). Contrary to most quantum MD methods that are based on effective single-particle wave functions, the DMFT approach is able to describe correlation-induced Mott metal-insulator transitions and the associated incoherent electronic excitations in an atomic liquid. We apply the DMFT-MD method to study Mott transitions in an atomic liquid model which can be viewed as the liquid-state generalization of the Hubbard model. The half-fille","authors_text":"Gia-Wei Chern, Zhijie Fan","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-08-18T15:40:46Z","title":"Atomistic simulation of Mott transition in fluid metals: Combining molecular dynamics with dynamical mean-field theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2208.08917","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":"sha256:2c7eeb43dd11f72eba80ae2df377d7d6f82c3137cbf2c92ba4af1644d1460d57","target":"record","created_at":"2026-07-05T04:49:39Z","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":"9f77d6145cc3e117e1538adb958816fed4cef26bd3b8576f50dbdaa2f3fa6554","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-08-18T15:40:46Z","title_canon_sha256":"deaefc621df1b55f5b05e590c3670834110ee8e9f2eeb9e4ea9cc451b93e2075"},"schema_version":"1.0","source":{"id":"2208.08917","kind":"arxiv","version":1}},"canonical_sha256":"b62f4afb4d0c96b9116887e87fef7d80313ba880e2af5ecaa1a9a597fddc6f88","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b62f4afb4d0c96b9116887e87fef7d80313ba880e2af5ecaa1a9a597fddc6f88","first_computed_at":"2026-07-05T04:49:39.715132Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:49:39.715132Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TYXhF/wiylp7IznpY6jwJyR5VCZWPC/6/uUEvS+ArNxnnp44mwHlfdQEnxLQsvG3qtXU+VJb83/tG3eIhENkDA==","signature_status":"signed_v1","signed_at":"2026-07-05T04:49:39.715548Z","signed_message":"canonical_sha256_bytes"},"source_id":"2208.08917","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2c7eeb43dd11f72eba80ae2df377d7d6f82c3137cbf2c92ba4af1644d1460d57","sha256:2845876548a432deb0a10853ff4ae5f5e29c081994cc2baf1f1c5a20f590ad9d"],"state_sha256":"1f9fb8c52eb64e67a0941a2bcdb36235ee03097f53e83cd0f66ffb0f21da0cd8"}