{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:MCNJTFPFXBCW7P23OCZJRUBJWA","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":"f827a208b81b308c9524264b16e3b225e381ef4bb997af93d1ad165eb066f877","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2018-12-31T23:59:31Z","title_canon_sha256":"7e8dc3ed87980cc5e8b65ebea3b81ac4e2c24886539accfe15d7f6c69ff60738"},"schema_version":"1.0","source":{"id":"1901.00065","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1901.00065","created_at":"2026-05-17T23:57:07Z"},{"alias_kind":"arxiv_version","alias_value":"1901.00065v1","created_at":"2026-05-17T23:57:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.00065","created_at":"2026-05-17T23:57:07Z"},{"alias_kind":"pith_short_12","alias_value":"MCNJTFPFXBCW","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_16","alias_value":"MCNJTFPFXBCW7P23","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_8","alias_value":"MCNJTFPF","created_at":"2026-05-18T12:32:37Z"}],"graph_snapshots":[{"event_id":"sha256:786bba2d884433db45031bcf6d497cb57e703f1a5aafb4d8237a41a9b3440e56","target":"graph","created_at":"2026-05-17T23:57:07Z","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":"Recent experiments of thin films flowing down a vertical fiber with varying nozzle diameters present a wealth of new dynamics that illustrate the need for more advanced theory. We present a detailed analysis using a full lubrication model that includes slip boundary conditions, nonlinear curvature terms, and a film stabilization term. This study brings to focus the presence of a stable liquid layer playing an important role in the full dynamics. We propose a combination of these physical effects to explain the observed velocity and stability of traveling droplets in the experiments and their t","authors_text":"A. L. Bertozzi, A. Sadeghpour, C. Falcon, H. Ji, Y. S. Ju, Z. Zeng","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2018-12-31T23:59:31Z","title":"Dynamics of thin liquid films on vertical cylindrical fibers"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.00065","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:cc457d58f779a4ae52beadf1ca98ef51471882fd5cab2355242d7a95f47fbe89","target":"record","created_at":"2026-05-17T23:57:07Z","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":"f827a208b81b308c9524264b16e3b225e381ef4bb997af93d1ad165eb066f877","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2018-12-31T23:59:31Z","title_canon_sha256":"7e8dc3ed87980cc5e8b65ebea3b81ac4e2c24886539accfe15d7f6c69ff60738"},"schema_version":"1.0","source":{"id":"1901.00065","kind":"arxiv","version":1}},"canonical_sha256":"609a9995e5b8456fbf5b70b298d029b015f274ba369402b47190b0a02c17671e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"609a9995e5b8456fbf5b70b298d029b015f274ba369402b47190b0a02c17671e","first_computed_at":"2026-05-17T23:57:07.008208Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:57:07.008208Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"S4aNVUqag4bjBiRrMlvXCXJCOK4FPIl71pHQWXgO3mYpy1EaWDDM+d4dojrZf+Gd6T8PIZjj8Dcio/f0kWcRDA==","signature_status":"signed_v1","signed_at":"2026-05-17T23:57:07.008579Z","signed_message":"canonical_sha256_bytes"},"source_id":"1901.00065","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cc457d58f779a4ae52beadf1ca98ef51471882fd5cab2355242d7a95f47fbe89","sha256:786bba2d884433db45031bcf6d497cb57e703f1a5aafb4d8237a41a9b3440e56"],"state_sha256":"29150c0e771f47ec60b73e1c24c6b64289e8718c9ce1a9ced96d2357e1ac3862"}