{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:SGCGJS74SZGIC446RODKE2NV4Y","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":"ef3184975a1735e47d0d099e84e899e4350d22e2e9225a5489999dbe7e188d46","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2025-02-11T15:01:54Z","title_canon_sha256":"9db8b2f841d07eab0292706326d7cd944af8bdf8ffb80eb928a573dfd9cb9b11"},"schema_version":"1.0","source":{"id":"2502.07610","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.07610","created_at":"2026-07-05T10:12:39Z"},{"alias_kind":"arxiv_version","alias_value":"2502.07610v1","created_at":"2026-07-05T10:12:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.07610","created_at":"2026-07-05T10:12:39Z"},{"alias_kind":"pith_short_12","alias_value":"SGCGJS74SZGI","created_at":"2026-07-05T10:12:39Z"},{"alias_kind":"pith_short_16","alias_value":"SGCGJS74SZGIC446","created_at":"2026-07-05T10:12:39Z"},{"alias_kind":"pith_short_8","alias_value":"SGCGJS74","created_at":"2026-07-05T10:12:39Z"}],"graph_snapshots":[{"event_id":"sha256:f844adf9d49e7735c785007e48aaf779811fb4cfee66068c2b7369a18e98b050","target":"graph","created_at":"2026-07-05T10:12:39Z","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/2502.07610/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this work we present a framework to explain the prediction of the velocity fluctuation at a certain wall-normal distance from wall measurements with a deep-learning model. For this purpose, we apply the deep-SHAP method to explain the velocity fluctuation prediction in wall-parallel planes in a turbulent open channel at a friction Reynolds number ${\\rm{Re}}_\\tau=180$. The explainable-deep-learning methodology comprises two stages. The first stage consists of training the estimator. In this case, the velocity fluctuation at a wall-normal distance of 15 wall units is predicted from the wall-s","authors_text":"A. Cremades, A. Ianiro, R. Freibergs, R. Vinuesa, S. Discetti, S. Hoyas","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2025-02-11T15:01:54Z","title":"Assessment of non-intrusive sensing in wall-bounded turbulence through explainable deep learning"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.07610","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":"sha256:16fa6438b3d72e742efe0ddf2ff708376ac9f09e01e1ed7ffd2570a5b84bc8fa","target":"record","created_at":"2026-07-05T10:12:39Z","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":"ef3184975a1735e47d0d099e84e899e4350d22e2e9225a5489999dbe7e188d46","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2025-02-11T15:01:54Z","title_canon_sha256":"9db8b2f841d07eab0292706326d7cd944af8bdf8ffb80eb928a573dfd9cb9b11"},"schema_version":"1.0","source":{"id":"2502.07610","kind":"arxiv","version":1}},"canonical_sha256":"918464cbfc964c81739e8b86a269b5e61e77e48f4e1a4f23933a07cf4b57d425","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"918464cbfc964c81739e8b86a269b5e61e77e48f4e1a4f23933a07cf4b57d425","first_computed_at":"2026-07-05T10:12:39.999445Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:12:39.999445Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"eqHvwavM8beUuLsPryU4zTvqqghVUErKXrUGhiy3Gx7nRN3ourTJpngEJtCTLMPWN8tk7BUBA+yT7Oi9uKAOCw==","signature_status":"signed_v1","signed_at":"2026-07-05T10:12:39.999949Z","signed_message":"canonical_sha256_bytes"},"source_id":"2502.07610","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:16fa6438b3d72e742efe0ddf2ff708376ac9f09e01e1ed7ffd2570a5b84bc8fa","sha256:f844adf9d49e7735c785007e48aaf779811fb4cfee66068c2b7369a18e98b050"],"state_sha256":"eb10b0bce0f2303728656793b07010d044c0612bc3db976a20c25f87dfbe3af1"}