{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:LVCSUTIXPMXBXB4XQV4BBDCIYF","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":"2d92bb80a3b6d4e7d6362f0351224b237c78f1ae51c0fd774c80d8e674a8ef5a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2020-07-13T16:47:19Z","title_canon_sha256":"46fe5c806f6d5a4879d51a57e2306d59dc9313376752a1e04cc9948c335641d1"},"schema_version":"1.0","source":{"id":"2007.06497","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2007.06497","created_at":"2026-07-05T02:59:47Z"},{"alias_kind":"arxiv_version","alias_value":"2007.06497v3","created_at":"2026-07-05T02:59:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2007.06497","created_at":"2026-07-05T02:59:47Z"},{"alias_kind":"pith_short_12","alias_value":"LVCSUTIXPMXB","created_at":"2026-07-05T02:59:47Z"},{"alias_kind":"pith_short_16","alias_value":"LVCSUTIXPMXBXB4X","created_at":"2026-07-05T02:59:47Z"},{"alias_kind":"pith_short_8","alias_value":"LVCSUTIX","created_at":"2026-07-05T02:59:47Z"}],"graph_snapshots":[{"event_id":"sha256:a11bf87f2bcc044e92d8a52af38b6dd84a3fcaf4f5eaf8d13070a3e21d1b3c97","target":"graph","created_at":"2026-07-05T02:59:47Z","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/2007.06497/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We use direct numerical simulation to study the temporal evolution of a perturbation localized on the turbulent layer that typically separates a cloud from the surrounding clear air. Across this shearless layer, a turbulent kinetic energy gradient naturally forms. Here, a finite perturbation in the form of a local initial temperature fluctuation is applied to simulate a hydrodynamic instability inside the background turbulent air flow. A numerical initial value problem for two diametrically opposite types of drop population distributions is then solved. Specifically, we consider a mono-dispers","authors_text":"Daniela Tordella, Federico Fraternale, Marco Vanni, Mattia Tomatis, Mina Golshan, Shahbozbek Abdunabiev","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2020-07-13T16:47:19Z","title":"Intermittency acceleration of water droplet population dynamics inside the interfacial layer between cloudy and clear air environments"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2007.06497","kind":"arxiv","version":3},"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":"sha256:2be5909e0a4ca906cb6191bdd6f8e7aafbe799c51fef1ba633a63388e82515f6","target":"record","created_at":"2026-07-05T02:59:47Z","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":"2d92bb80a3b6d4e7d6362f0351224b237c78f1ae51c0fd774c80d8e674a8ef5a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2020-07-13T16:47:19Z","title_canon_sha256":"46fe5c806f6d5a4879d51a57e2306d59dc9313376752a1e04cc9948c335641d1"},"schema_version":"1.0","source":{"id":"2007.06497","kind":"arxiv","version":3}},"canonical_sha256":"5d452a4d177b2e1b87978578108c48c1530058ab7e0d930ea8475215a9dece8f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5d452a4d177b2e1b87978578108c48c1530058ab7e0d930ea8475215a9dece8f","first_computed_at":"2026-07-05T02:59:47.167385Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:59:47.167385Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"oCAkwjzgx72P0Koz2Esk5Hmqmre6346hhpbNc5k7jTgPdmrOj0Gv8n0NuCLcr2MiwfYuim6EgxdPkmiKirGMAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T02:59:47.167886Z","signed_message":"canonical_sha256_bytes"},"source_id":"2007.06497","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2be5909e0a4ca906cb6191bdd6f8e7aafbe799c51fef1ba633a63388e82515f6","sha256:a11bf87f2bcc044e92d8a52af38b6dd84a3fcaf4f5eaf8d13070a3e21d1b3c97"],"state_sha256":"171a2f89660dab404ad205053790c2e008cca2af3315772551bc56b08b1e1afa"}