{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:FXVRWAPEF76M6AOIKVKXT6INF2","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":"6d472006e4e4e3d8aa62cd4a294538d04310390d3990b634df8dad26027b3bbb","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.soft","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-16T11:28:20Z","title_canon_sha256":"2e88f295584b716bbfa19873eeaee2b46062ed90cabf261e6a4735697d50869d"},"schema_version":"1.0","source":{"id":"2305.09357","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2305.09357","created_at":"2026-07-05T06:10:47Z"},{"alias_kind":"arxiv_version","alias_value":"2305.09357v1","created_at":"2026-07-05T06:10:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.09357","created_at":"2026-07-05T06:10:47Z"},{"alias_kind":"pith_short_12","alias_value":"FXVRWAPEF76M","created_at":"2026-07-05T06:10:47Z"},{"alias_kind":"pith_short_16","alias_value":"FXVRWAPEF76M6AOI","created_at":"2026-07-05T06:10:47Z"},{"alias_kind":"pith_short_8","alias_value":"FXVRWAPE","created_at":"2026-07-05T06:10:47Z"}],"graph_snapshots":[{"event_id":"sha256:6d2ce6d7dd96a89c4cb5047c381afaf7565e70fe4a41e9134d0a556c900dc066","target":"graph","created_at":"2026-07-05T06:10:47Z","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/2305.09357/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The complete quantitative description of the structure of dense and supercooled liquids remains a notoriously difficult problem in statistical physics. Most studies to date focus solely on two-body structural correlations, and only a handful of papers have sought to consider additional three-body correlations. Here, we go beyond the state of the art by extracting many-body static structure factors from molecular dynamics simulations and by deriving accurate approximations up to the six-body structure factor via density functional theory. We find that supercooling manifestly increases four-body","authors_text":"Chengjie Luo, Corentin C.L. Laudicina, Ilian Pihlajamaa, Liesbeth M.C. Janssen","cross_cats":["cond-mat.dis-nn","cond-mat.soft","physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-16T11:28:20Z","title":"Emergent structural correlations in dense liquids"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.09357","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":"sha256:816d6ce39cb1f311d89d88aa694c5206b96a7073d23e5cf1d9ae173c0bc311b7","target":"record","created_at":"2026-07-05T06:10:47Z","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":"6d472006e4e4e3d8aa62cd4a294538d04310390d3990b634df8dad26027b3bbb","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.soft","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-05-16T11:28:20Z","title_canon_sha256":"2e88f295584b716bbfa19873eeaee2b46062ed90cabf261e6a4735697d50869d"},"schema_version":"1.0","source":{"id":"2305.09357","kind":"arxiv","version":1}},"canonical_sha256":"2deb1b01e42ffccf01c8555579f90d2eb927d5a52ac39b6f248d8403068d0ce0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2deb1b01e42ffccf01c8555579f90d2eb927d5a52ac39b6f248d8403068d0ce0","first_computed_at":"2026-07-05T06:10:47.199365Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:10:47.199365Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/trY34GDdSlFQRgA3+m6VZQ2Cyl2yCDpGVLiMYtNHQNJgBBdmnp5JdS7qt6JDUJH8iL1jXyna50ivHpQp2VpAA==","signature_status":"signed_v1","signed_at":"2026-07-05T06:10:47.199772Z","signed_message":"canonical_sha256_bytes"},"source_id":"2305.09357","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:816d6ce39cb1f311d89d88aa694c5206b96a7073d23e5cf1d9ae173c0bc311b7","sha256:6d2ce6d7dd96a89c4cb5047c381afaf7565e70fe4a41e9134d0a556c900dc066"],"state_sha256":"71d4f06d30bcdaa24910e496acf7ef8ca66726d56267fcb2aa51dae65238637c"}