{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:QFPFKCWVIWJ67V6RY6K4LOVOC7","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":"8f53c3fb3489226c8004f40edfbc659725713bfa773f3f70ce0140691fcda2c4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2010-10-08T23:25:08Z","title_canon_sha256":"3e342115b4a89770d25b5d02a2eaff530159da45461bd4617b0484335268a4d5"},"schema_version":"1.0","source":{"id":"1010.1795","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.1795","created_at":"2026-05-18T04:39:38Z"},{"alias_kind":"arxiv_version","alias_value":"1010.1795v1","created_at":"2026-05-18T04:39:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.1795","created_at":"2026-05-18T04:39:38Z"},{"alias_kind":"pith_short_12","alias_value":"QFPFKCWVIWJ6","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_16","alias_value":"QFPFKCWVIWJ67V6R","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_8","alias_value":"QFPFKCWV","created_at":"2026-05-18T12:26:12Z"}],"graph_snapshots":[{"event_id":"sha256:267cd701ffd2957179b32a7fb9d8ac8c4f03117f2676d38f3fe9a8ba3a0fe2ab","target":"graph","created_at":"2026-05-18T04:39:38Z","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":"This fluid dynamics video shows the breakup of a droplet in a stationary homogeneous and isotropic turbulent flow. We consider droplets with the same density of the transporting fluid. The droplets and the fluid are numerically modelled by means of a multicompo- nent Lattice-Boltzmann method. The turbulent fluid is maintained through a large scale stirring force and the radius of stable droplets, for the parameters in our simulation, is larger than the Kolmogorov scale. Events of droplet deformation, break-up and aggregation are clearly visible from the movie. With the present database droplet","authors_text":"Federico Toschi, Luca Biferale, Mauro Sbragaglia, Prasad Perlekar","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2010-10-08T23:25:08Z","title":"Droplet breakup in homogeneous and isotropic turbulence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.1795","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":"sha256:3bb70471f7d16e74f53d86ab0796aebe7175a11c57ba69091003821d8dd2b6b9","target":"record","created_at":"2026-05-18T04:39:38Z","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":"8f53c3fb3489226c8004f40edfbc659725713bfa773f3f70ce0140691fcda2c4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2010-10-08T23:25:08Z","title_canon_sha256":"3e342115b4a89770d25b5d02a2eaff530159da45461bd4617b0484335268a4d5"},"schema_version":"1.0","source":{"id":"1010.1795","kind":"arxiv","version":1}},"canonical_sha256":"815e550ad54593efd7d1c795c5baae17ebe8fb00b50458aff1f4b0814128279e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"815e550ad54593efd7d1c795c5baae17ebe8fb00b50458aff1f4b0814128279e","first_computed_at":"2026-05-18T04:39:38.504188Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:39:38.504188Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zk25GWYgCMn/lVGfLGgrXX/2CRs39EuJuFMOFB6gJ2eDdNci3obTYGClbWGvf1CViPMb08O6pNE0kUnuJqXYBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:39:38.504636Z","signed_message":"canonical_sha256_bytes"},"source_id":"1010.1795","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3bb70471f7d16e74f53d86ab0796aebe7175a11c57ba69091003821d8dd2b6b9","sha256:267cd701ffd2957179b32a7fb9d8ac8c4f03117f2676d38f3fe9a8ba3a0fe2ab"],"state_sha256":"a3f8a91f21f1162b6362c9b46f35e5d25e1669560c09536c1cc976a792013824"}