{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:DZKS5T6J7EMLPKNZ7ODM232YBX","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":"e68021eb8942349373a71ce36c7dc3e359ebfa9a01d9feff84faff2ef68c066f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2020-05-12T09:19:11Z","title_canon_sha256":"51d24039f3f7a603f5ec87ab34547708818f40a6e9b15304b4308fd05f2b1158"},"schema_version":"1.0","source":{"id":"2005.05633","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2005.05633","created_at":"2026-07-05T04:25:34Z"},{"alias_kind":"arxiv_version","alias_value":"2005.05633v2","created_at":"2026-07-05T04:25:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2005.05633","created_at":"2026-07-05T04:25:34Z"},{"alias_kind":"pith_short_12","alias_value":"DZKS5T6J7EML","created_at":"2026-07-05T04:25:34Z"},{"alias_kind":"pith_short_16","alias_value":"DZKS5T6J7EMLPKNZ","created_at":"2026-07-05T04:25:34Z"},{"alias_kind":"pith_short_8","alias_value":"DZKS5T6J","created_at":"2026-07-05T04:25:34Z"}],"graph_snapshots":[{"event_id":"sha256:279f3d2105983303096dd9f253de5ddaca0913cffabe3d8d8e66847e8d29e726","target":"graph","created_at":"2026-07-05T04:25:34Z","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/2005.05633/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"It is commonly accepted that the breakup criteria of drops or bubbles in turbulence is governed by surface tension and inertia. However, also {\\it{buoyancy}} can play an important role at breakup. In order to better understand this role, here we numerically study Rayleigh-B\\'enard convection for two immiscible fluid layers, in order to identify the effects of buoyancy on interface breakup. We explore the parameter space spanned by the Weber number $5\\leq We \\leq 5000$ (the ratio of inertia to surface tension) and the density ratio between the two fluids $0.001 \\leq \\Lambda \\leq 1$, at fixed Ra","authors_text":"Chong Shen Ng, Detlef Lohse, Hao-Ran Liu, Kai Leong Chong, Qi Wang, Roberto Verzicco","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2020-05-12T09:19:11Z","title":"Two-layer Thermally Driven Turbulence: Mechanisms for Interface Breakup"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2005.05633","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":"sha256:7aa491ff2f1002824c4f73166652d66b4b8a85c7d0e1370f751370aa74f77c14","target":"record","created_at":"2026-07-05T04:25:34Z","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":"e68021eb8942349373a71ce36c7dc3e359ebfa9a01d9feff84faff2ef68c066f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2020-05-12T09:19:11Z","title_canon_sha256":"51d24039f3f7a603f5ec87ab34547708818f40a6e9b15304b4308fd05f2b1158"},"schema_version":"1.0","source":{"id":"2005.05633","kind":"arxiv","version":2}},"canonical_sha256":"1e552ecfc9f918b7a9b9fb86cd6f580dc74817c8df2e5abc8ffcfa9917c96e50","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1e552ecfc9f918b7a9b9fb86cd6f580dc74817c8df2e5abc8ffcfa9917c96e50","first_computed_at":"2026-07-05T04:25:34.133861Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:25:34.133861Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NcXlpx0gXsjZOY/1glWLSFwoKifWHBfZTq8+GDXW4inkSkhDszd8FdhKwAI+oyidPgiXIKCM873iNuIVmsIzCA==","signature_status":"signed_v1","signed_at":"2026-07-05T04:25:34.134265Z","signed_message":"canonical_sha256_bytes"},"source_id":"2005.05633","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7aa491ff2f1002824c4f73166652d66b4b8a85c7d0e1370f751370aa74f77c14","sha256:279f3d2105983303096dd9f253de5ddaca0913cffabe3d8d8e66847e8d29e726"],"state_sha256":"81856c18765de5ec0d6e4493062d6e10035a405dad4015c7480ddde14d0e0d7d"}