{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:JC7QIS7L6CPT5GWCQR7MDBHUHP","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":"2c9a60f3ff6fd7a3dbd19861621cd9c3f1a78776c353f61481ced51e419b5d93","cross_cats_sorted":["cond-mat.stat-mech","physics.chem-ph","physics.flu-dyn","physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2019-01-16T08:29:24Z","title_canon_sha256":"4e76c14af5f215d7f2c547c30efd9f9191a869a6b153473b7513745eb3c258f4"},"schema_version":"1.0","source":{"id":"1901.05175","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1901.05175","created_at":"2026-05-17T23:44:12Z"},{"alias_kind":"arxiv_version","alias_value":"1901.05175v2","created_at":"2026-05-17T23:44:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.05175","created_at":"2026-05-17T23:44:12Z"},{"alias_kind":"pith_short_12","alias_value":"JC7QIS7L6CPT","created_at":"2026-05-18T12:33:18Z"},{"alias_kind":"pith_short_16","alias_value":"JC7QIS7L6CPT5GWC","created_at":"2026-05-18T12:33:18Z"},{"alias_kind":"pith_short_8","alias_value":"JC7QIS7L","created_at":"2026-05-18T12:33:18Z"}],"graph_snapshots":[{"event_id":"sha256:dae6c615848a1bae30300b213aed748079d8f6c9604def17863f4d4bb3bad23c","target":"graph","created_at":"2026-05-17T23:44:12Z","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":"Determining the microstructure of colloidal suspensions under shear flows has been a challenge for theoretical and computational methods due to the singularly-perturbed boundary-layer nature of the problem. Previous approaches have been limited to the case of hard-sphere systems and suffer from various limitations in their applicability. We present a new analytic scheme based on intermediate asymptotics which solves the Smoluchowski diffusion-convection equation including both intermolecular and hydrodynamic interactions. The method is able to recover previous results for the hard-sphere fluid","authors_text":"A. Zaccone, L. Banetta","cross_cats":["cond-mat.stat-mech","physics.chem-ph","physics.flu-dyn","physics.plasm-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2019-01-16T08:29:24Z","title":"Radial distribution function of Lennard-Jones fluids in shear flows from intermediate asymptotics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.05175","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":"sha256:879ce5642409f251fe34b89c7b859526f8af375c33da919f28ecba956957647e","target":"record","created_at":"2026-05-17T23:44:12Z","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":"2c9a60f3ff6fd7a3dbd19861621cd9c3f1a78776c353f61481ced51e419b5d93","cross_cats_sorted":["cond-mat.stat-mech","physics.chem-ph","physics.flu-dyn","physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2019-01-16T08:29:24Z","title_canon_sha256":"4e76c14af5f215d7f2c547c30efd9f9191a869a6b153473b7513745eb3c258f4"},"schema_version":"1.0","source":{"id":"1901.05175","kind":"arxiv","version":2}},"canonical_sha256":"48bf044bebf09f3e9ac2847ec184f43bcb8675c8cfdfb7f662c1e83d5cac65d2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"48bf044bebf09f3e9ac2847ec184f43bcb8675c8cfdfb7f662c1e83d5cac65d2","first_computed_at":"2026-05-17T23:44:12.318105Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:44:12.318105Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MGo7Fwqma0gqGlwKKucDfqr32Th2sHXT9m7T4k4yTnbGpfej6HaRU2Qt7IqroiDKuf5trZCkezcOKVTbb5hfBw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:44:12.318706Z","signed_message":"canonical_sha256_bytes"},"source_id":"1901.05175","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:879ce5642409f251fe34b89c7b859526f8af375c33da919f28ecba956957647e","sha256:dae6c615848a1bae30300b213aed748079d8f6c9604def17863f4d4bb3bad23c"],"state_sha256":"94ab77de8519481cbd0e30932e8bdb267d9a41660a51764c82737317ac1944c7"}