{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:QJDTNOCZV67U7JY737LYOX45ZC","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":"18a08f702223d7b61c01ee5f59e0e32cd4b8084d355ff0f0803887caf8b934f2","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2022-03-25T13:23:33Z","title_canon_sha256":"5266c48d6a4dd5cef274d95207eddb5d945f8ae52be0087e8bee6583ddc790f6"},"schema_version":"1.0","source":{"id":"2203.13638","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2203.13638","created_at":"2026-07-05T04:08:34Z"},{"alias_kind":"arxiv_version","alias_value":"2203.13638v1","created_at":"2026-07-05T04:08:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2203.13638","created_at":"2026-07-05T04:08:34Z"},{"alias_kind":"pith_short_12","alias_value":"QJDTNOCZV67U","created_at":"2026-07-05T04:08:34Z"},{"alias_kind":"pith_short_16","alias_value":"QJDTNOCZV67U7JY7","created_at":"2026-07-05T04:08:34Z"},{"alias_kind":"pith_short_8","alias_value":"QJDTNOCZ","created_at":"2026-07-05T04:08:34Z"}],"graph_snapshots":[{"event_id":"sha256:a3433fc63d7fedb5db655a7ff7ffd365fde1106376c3a6ed89a102da137c0ca6","target":"graph","created_at":"2026-07-05T04:08:34Z","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/2203.13638/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We combine a heuristic theory of geometric percolation and the Smoluchowski theory of colloid dynamics to predict the impact of shear flow on the percolation threshold of hard spherical colloidal particles, and verify our findings by means of molecular dynamics simulations. It appears that the impact of shear flow is subtle and highly non-trivial, even in the absence of hydrodynamic interactions between the particles. The presence of shear flow can both increase and decrease the percolation threshold, depending on the criterion used for determining whether or not two particles are connected an","authors_text":"Ilian Pihlajamaa, Paul van der Schoot, Ren\\'e de Bruijn","cross_cats":["cond-mat.mtrl-sci","cond-mat.stat-mech","physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2022-03-25T13:23:33Z","title":"Geometric percolation of colloids in shear flow"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2203.13638","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":"sha256:91dab8f831a4549a4c84e910c540284932e42186f12eeb117eb3f156c52feff4","target":"record","created_at":"2026-07-05T04:08:34Z","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":"18a08f702223d7b61c01ee5f59e0e32cd4b8084d355ff0f0803887caf8b934f2","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2022-03-25T13:23:33Z","title_canon_sha256":"5266c48d6a4dd5cef274d95207eddb5d945f8ae52be0087e8bee6583ddc790f6"},"schema_version":"1.0","source":{"id":"2203.13638","kind":"arxiv","version":1}},"canonical_sha256":"824736b859afbf4fa71fdfd7875f9dc8988bfcf99b77bcc95732cb8ab11187fa","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"824736b859afbf4fa71fdfd7875f9dc8988bfcf99b77bcc95732cb8ab11187fa","first_computed_at":"2026-07-05T04:08:34.867773Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:08:34.867773Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qk4HvxIe5OYJKJqCUjY2Kn7rs6K/p1Js2GhkRNEMMmwbDuMeeAemb5tU/XdOMoFgBAFxRVYy9Q3pxzIqF0/JBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T04:08:34.868257Z","signed_message":"canonical_sha256_bytes"},"source_id":"2203.13638","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:91dab8f831a4549a4c84e910c540284932e42186f12eeb117eb3f156c52feff4","sha256:a3433fc63d7fedb5db655a7ff7ffd365fde1106376c3a6ed89a102da137c0ca6"],"state_sha256":"798fe8cf10e31fbccb48d27a26cc6d72cf66b3b61274130e04808599172928b1"}