{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:557MT7ZX7Z4S2I22RPQXOAFRER","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":"6e4a3dacff5607150f610e4904f97f0ddae8de695303bdca36c41580b6ca3f21","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2023-07-02T16:41:43Z","title_canon_sha256":"75ebd1e23a420d7c170a164c9fcda452e457927570d0f5277c68439bb20b1b89"},"schema_version":"1.0","source":{"id":"2307.00612","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2307.00612","created_at":"2026-07-05T06:56:35Z"},{"alias_kind":"arxiv_version","alias_value":"2307.00612v3","created_at":"2026-07-05T06:56:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2307.00612","created_at":"2026-07-05T06:56:35Z"},{"alias_kind":"pith_short_12","alias_value":"557MT7ZX7Z4S","created_at":"2026-07-05T06:56:35Z"},{"alias_kind":"pith_short_16","alias_value":"557MT7ZX7Z4S2I22","created_at":"2026-07-05T06:56:35Z"},{"alias_kind":"pith_short_8","alias_value":"557MT7ZX","created_at":"2026-07-05T06:56:35Z"}],"graph_snapshots":[{"event_id":"sha256:0e5df2da330b35bfac780cb3c59489a66cbeabf559d4fe53e3020ac721181f6f","target":"graph","created_at":"2026-07-05T06:56:35Z","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/2307.00612/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The scaling of Reynolds stresses in turbulent wall-bounded flows is the subject of a long running debate. In the near-wall ``inner'' region, a sizeable group, inspired by the ``attached eddy model'', has advocated the unlimited growth of $\\langle uu\\rangle^+$ and in particular of its inner peak at $y^+\\approxeq 15$, with $\\ln\\Reytau$ \\citep[see e.g.][and references therein]{smitsetal2021}. Only recently, \\citet{chen_sreeni2021,chen_sreeni2022} have argued on the basis of bounded dissipation, that $\\langle uu\\rangle^+$ remains finite in the inner near-wall region for $\\Reytau\\rightarrow\\infty$,","authors_text":"Peter A. Monkewitz","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2023-07-02T16:41:43Z","title":"Reynolds number scaling and inner-outer overlap of stream-wise Reynolds stress in wall turbulence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2307.00612","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":"sha256:90d03a372bc3d72446b4fa22c9acac7beebdfdf877bcdc098358745b743321dd","target":"record","created_at":"2026-07-05T06:56:35Z","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":"6e4a3dacff5607150f610e4904f97f0ddae8de695303bdca36c41580b6ca3f21","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2023-07-02T16:41:43Z","title_canon_sha256":"75ebd1e23a420d7c170a164c9fcda452e457927570d0f5277c68439bb20b1b89"},"schema_version":"1.0","source":{"id":"2307.00612","kind":"arxiv","version":3}},"canonical_sha256":"ef7ec9ff37fe792d235a8be17700b12455dc3a046749bf41e76aa657dc8a7ea6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ef7ec9ff37fe792d235a8be17700b12455dc3a046749bf41e76aa657dc8a7ea6","first_computed_at":"2026-07-05T06:56:35.624707Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:56:35.624707Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Dq+6OvVRTxAMKi7RFG63LSOBxcIzyOIZNOCtfCnuHHfMoJMV29qfld35WiMezHqXe/LHY4aeCN/9Yhkr+GFNBA==","signature_status":"signed_v1","signed_at":"2026-07-05T06:56:35.625216Z","signed_message":"canonical_sha256_bytes"},"source_id":"2307.00612","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:90d03a372bc3d72446b4fa22c9acac7beebdfdf877bcdc098358745b743321dd","sha256:0e5df2da330b35bfac780cb3c59489a66cbeabf559d4fe53e3020ac721181f6f"],"state_sha256":"1cd37d9b34dbe4e0404643f575e1d4c243c15704a5e634b9cfb9c3e4ff0c8102"}