{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:HOMTVLPILO4YDRLPNGSG5MFODA","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":"4d7586d0755bef19306888fcedfdd2bf734353d0eb4a5a39605880ced3404a64","cross_cats_sorted":["math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2023-03-29T00:57:57Z","title_canon_sha256":"154b292598fc959ac24ebb5c6cc2b9e1e70b0a6a43aeabd1d6f9d3cdd70a30e0"},"schema_version":"1.0","source":{"id":"2303.16374","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2303.16374","created_at":"2026-07-05T05:56:06Z"},{"alias_kind":"arxiv_version","alias_value":"2303.16374v1","created_at":"2026-07-05T05:56:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2303.16374","created_at":"2026-07-05T05:56:06Z"},{"alias_kind":"pith_short_12","alias_value":"HOMTVLPILO4Y","created_at":"2026-07-05T05:56:06Z"},{"alias_kind":"pith_short_16","alias_value":"HOMTVLPILO4YDRLP","created_at":"2026-07-05T05:56:06Z"},{"alias_kind":"pith_short_8","alias_value":"HOMTVLPI","created_at":"2026-07-05T05:56:06Z"}],"graph_snapshots":[{"event_id":"sha256:b03b0f270f69f1e15d19a6dee2f61f93f187f80ed0a500ae0757b3986f6fa7a2","target":"graph","created_at":"2026-07-05T05:56:06Z","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/2303.16374/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Very recently, a defect model which depicts the growth tendency of the near-wall peak of the streamwise turbulence intensity has been developed (Chen $\\&$ Sreenivasan, J. Fluid Mech. (2021), vol.908, R3). Based on the finiteness of the near-wall turbulence production, this model predicts that the magnitude of the peak will approach a finite limit as the Reynolds number increases. In the present study, we revisit the basic hypotheses of the model, such as the balance between the turbulence production and the wall dissipation in the region of peak production, the negligible effects of the logari","authors_text":"Cheng cheng, Lin Fu","cross_cats":["math-ph","math.MP"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2023-03-29T00:57:57Z","title":"A scale-based study of the Reynolds number scaling for the near-wall streamwise turbulence intensity in wall turbulence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.16374","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":"sha256:7aad2a579200b8645c47fb2a7bdbf267b5d4ccea5feca7086868555f4d9c1bed","target":"record","created_at":"2026-07-05T05:56:06Z","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":"4d7586d0755bef19306888fcedfdd2bf734353d0eb4a5a39605880ced3404a64","cross_cats_sorted":["math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2023-03-29T00:57:57Z","title_canon_sha256":"154b292598fc959ac24ebb5c6cc2b9e1e70b0a6a43aeabd1d6f9d3cdd70a30e0"},"schema_version":"1.0","source":{"id":"2303.16374","kind":"arxiv","version":1}},"canonical_sha256":"3b993aade85bb981c56f69a46eb0ae181024b675f81c35b480c99178df5892a9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3b993aade85bb981c56f69a46eb0ae181024b675f81c35b480c99178df5892a9","first_computed_at":"2026-07-05T05:56:06.113386Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:56:06.113386Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"LpgrNiXJGFgArkNWQ3W+aOuM5aNge0h60OsTR9il0XFaF9Z7a9IRarbaj8UHW8IAviBlGsCBPmEWj6iTD8LwAg==","signature_status":"signed_v1","signed_at":"2026-07-05T05:56:06.113786Z","signed_message":"canonical_sha256_bytes"},"source_id":"2303.16374","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7aad2a579200b8645c47fb2a7bdbf267b5d4ccea5feca7086868555f4d9c1bed","sha256:b03b0f270f69f1e15d19a6dee2f61f93f187f80ed0a500ae0757b3986f6fa7a2"],"state_sha256":"e5ad1a5d2b4d583eebaaff1acb49b6ed90888c7f322207471ad4d90e8db73a8f"}