{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:OKLD7EEPP3R4XRO3FMF5DGYGGJ","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":"4b6a9654eaaf50f8fb1c3b24d7d3a807dfe6e092f95165cb0094c330ce1c2ff3","cross_cats_sorted":["physics.flu-dyn"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-07T17:01:29Z","title_canon_sha256":"057f20e8959403d2b998c990fda9c3d894ec860ffd23654578de0cfca0ce2b4a"},"schema_version":"1.0","source":{"id":"2606.08732","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.08732","created_at":"2026-06-09T02:07:36Z"},{"alias_kind":"arxiv_version","alias_value":"2606.08732v1","created_at":"2026-06-09T02:07:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.08732","created_at":"2026-06-09T02:07:36Z"},{"alias_kind":"pith_short_12","alias_value":"OKLD7EEPP3R4","created_at":"2026-06-09T02:07:36Z"},{"alias_kind":"pith_short_16","alias_value":"OKLD7EEPP3R4XRO3","created_at":"2026-06-09T02:07:36Z"},{"alias_kind":"pith_short_8","alias_value":"OKLD7EEP","created_at":"2026-06-09T02:07:36Z"}],"graph_snapshots":[{"event_id":"sha256:ec1da95e500a9c93cfcf5df4229d7751dac4ff402afdeb89438e661a477db05f","target":"graph","created_at":"2026-06-09T02:07:36Z","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/2606.08732/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Wave resistance is the drag generated by the wave radiation that a source moving at a fluid interface sustains. Under stochastic trajectories, the mean drag is controlled by the ensemble-averaged surface profile built from the trajectory history. We show that the result is a finite resistance below the deterministic radiation threshold and a regularization of the singular response at the minimum phase velocity of the capillary-gravity waves. We derive explicit scaling laws for drifted Brownian trajectories, including a universal high-diffusivity decay. For drifted L\\'evy flight, we find the me","authors_text":"Elie Raphael, Maxence Arutkin, Shlomi Reuveni","cross_cats":["physics.flu-dyn"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-07T17:01:29Z","title":"Wave Resistance for Stochastic Motion at Interfaces"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.08732","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":"sha256:7f11c2618743f501a5cdf6ba7151dc3a5cd75f793bffdcb037f25e019883478d","target":"record","created_at":"2026-06-09T02:07:36Z","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":"4b6a9654eaaf50f8fb1c3b24d7d3a807dfe6e092f95165cb0094c330ce1c2ff3","cross_cats_sorted":["physics.flu-dyn"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-07T17:01:29Z","title_canon_sha256":"057f20e8959403d2b998c990fda9c3d894ec860ffd23654578de0cfca0ce2b4a"},"schema_version":"1.0","source":{"id":"2606.08732","kind":"arxiv","version":1}},"canonical_sha256":"72963f908f7ee3cbc5db2b0bd19b06327a7a524753a9f2d04d3748a1a26aa7d4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"72963f908f7ee3cbc5db2b0bd19b06327a7a524753a9f2d04d3748a1a26aa7d4","first_computed_at":"2026-06-09T02:07:36.080280Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-09T02:07:36.080280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"68xdFVN8cyHWbVC819IZPyEkh6vBqOIKI4jfUCAbWQhOjmbFbmxwsIEVC10oquomD4N7xI3IssZhq6fsg86ZAw==","signature_status":"signed_v1","signed_at":"2026-06-09T02:07:36.080982Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.08732","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7f11c2618743f501a5cdf6ba7151dc3a5cd75f793bffdcb037f25e019883478d","sha256:ec1da95e500a9c93cfcf5df4229d7751dac4ff402afdeb89438e661a477db05f"],"state_sha256":"93fc7e2f3c35d9288d4ad5bf8838d4d10552c6d46dc45c62c77eaffa642b03e2"}