{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:5AIUI3LZT6OYHJ5XLA3L4RKY4X","short_pith_number":"pith:5AIUI3LZ","schema_version":"1.0","canonical_sha256":"e811446d799f9d83a7b75836be4558e5fed1f27c2dc826d44a26250a8b27811b","source":{"kind":"arxiv","id":"2606.06876","version":1},"attestation_state":"computed","paper":{"title":"A Wall Function for Turbulent Boundary Layers under Rotation via Symbolic Regression","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Haiwang Li, Ruquan You, Yao Ma, Zhi Tao","submitted_at":"2026-06-05T03:43:54Z","abstract_excerpt":"This study employs symbolic regression to derive physically interpretable, white-box wall-function expressions for turbulent boundary layers under system rotation. Flows in a rotating frame are subject to Coriolis forces, which deflect the boundary layer profile from static case. The classical law of the wall, formulated under non-rotating conditions, is ill-suited to describing the effects of rotation. To obtain the wall function under rotation, we examine the deflection behavior of the turbulent boundary layers on the leading and trailing sides, and construct wall functions that are valid ov"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2606.06876","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2026-06-05T03:43:54Z","cross_cats_sorted":[],"title_canon_sha256":"3d4aad99cec03410d88ab644fbbfea067e07658074c0e231f943269c0124b405","abstract_canon_sha256":"326fa951002183dc16776a012904ee7d903cdb89585593c783eb7505fe335147"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-08T01:04:33.456887Z","signature_b64":"Wy5UoimlNxElynaekTGZezPfISr5kLC/bGrbYm8xTYNb2aPkem5Vb26sjomBtD+/7AdAeAa5IBwPj7roCHUcBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e811446d799f9d83a7b75836be4558e5fed1f27c2dc826d44a26250a8b27811b","last_reissued_at":"2026-06-08T01:04:33.456173Z","signature_status":"signed_v1","first_computed_at":"2026-06-08T01:04:33.456173Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Wall Function for Turbulent Boundary Layers under Rotation via Symbolic Regression","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Haiwang Li, Ruquan You, Yao Ma, Zhi Tao","submitted_at":"2026-06-05T03:43:54Z","abstract_excerpt":"This study employs symbolic regression to derive physically interpretable, white-box wall-function expressions for turbulent boundary layers under system rotation. Flows in a rotating frame are subject to Coriolis forces, which deflect the boundary layer profile from static case. The classical law of the wall, formulated under non-rotating conditions, is ill-suited to describing the effects of rotation. To obtain the wall function under rotation, we examine the deflection behavior of the turbulent boundary layers on the leading and trailing sides, and construct wall functions that are valid ov"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.06876","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2606.06876/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2606.06876","created_at":"2026-06-08T01:04:33.456289+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.06876v1","created_at":"2026-06-08T01:04:33.456289+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.06876","created_at":"2026-06-08T01:04:33.456289+00:00"},{"alias_kind":"pith_short_12","alias_value":"5AIUI3LZT6OY","created_at":"2026-06-08T01:04:33.456289+00:00"},{"alias_kind":"pith_short_16","alias_value":"5AIUI3LZT6OYHJ5X","created_at":"2026-06-08T01:04:33.456289+00:00"},{"alias_kind":"pith_short_8","alias_value":"5AIUI3LZ","created_at":"2026-06-08T01:04:33.456289+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5AIUI3LZT6OYHJ5XLA3L4RKY4X","json":"https://pith.science/pith/5AIUI3LZT6OYHJ5XLA3L4RKY4X.json","graph_json":"https://pith.science/api/pith-number/5AIUI3LZT6OYHJ5XLA3L4RKY4X/graph.json","events_json":"https://pith.science/api/pith-number/5AIUI3LZT6OYHJ5XLA3L4RKY4X/events.json","paper":"https://pith.science/paper/5AIUI3LZ"},"agent_actions":{"view_html":"https://pith.science/pith/5AIUI3LZT6OYHJ5XLA3L4RKY4X","download_json":"https://pith.science/pith/5AIUI3LZT6OYHJ5XLA3L4RKY4X.json","view_paper":"https://pith.science/paper/5AIUI3LZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.06876&json=true","fetch_graph":"https://pith.science/api/pith-number/5AIUI3LZT6OYHJ5XLA3L4RKY4X/graph.json","fetch_events":"https://pith.science/api/pith-number/5AIUI3LZT6OYHJ5XLA3L4RKY4X/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5AIUI3LZT6OYHJ5XLA3L4RKY4X/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5AIUI3LZT6OYHJ5XLA3L4RKY4X/action/storage_attestation","attest_author":"https://pith.science/pith/5AIUI3LZT6OYHJ5XLA3L4RKY4X/action/author_attestation","sign_citation":"https://pith.science/pith/5AIUI3LZT6OYHJ5XLA3L4RKY4X/action/citation_signature","submit_replication":"https://pith.science/pith/5AIUI3LZT6OYHJ5XLA3L4RKY4X/action/replication_record"}},"created_at":"2026-06-08T01:04:33.456289+00:00","updated_at":"2026-06-08T01:04:33.456289+00:00"}