{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:DUTPJOF6MKUJNE5FQBGBL4HJK2","short_pith_number":"pith:DUTPJOF6","canonical_record":{"source":{"id":"2407.11206","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-07-15T19:41:00Z","cross_cats_sorted":[],"title_canon_sha256":"536ef8f106ae4a293ed375d62f739534323fdf99d9b8bf450ff1fb84519c3985","abstract_canon_sha256":"f3589c0114a273458ab2c81c96edfe9084685e4253954eb4bdc1a8df5cedbdaf"},"schema_version":"1.0"},"canonical_sha256":"1d26f4b8be62a89693a5804c15f0e956a1b8f80f29e441f0a01b0ba1f3c0af99","source":{"kind":"arxiv","id":"2407.11206","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2407.11206","created_at":"2026-07-05T10:18:39Z"},{"alias_kind":"arxiv_version","alias_value":"2407.11206v2","created_at":"2026-07-05T10:18:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2407.11206","created_at":"2026-07-05T10:18:39Z"},{"alias_kind":"pith_short_12","alias_value":"DUTPJOF6MKUJ","created_at":"2026-07-05T10:18:39Z"},{"alias_kind":"pith_short_16","alias_value":"DUTPJOF6MKUJNE5F","created_at":"2026-07-05T10:18:39Z"},{"alias_kind":"pith_short_8","alias_value":"DUTPJOF6","created_at":"2026-07-05T10:18:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:DUTPJOF6MKUJNE5FQBGBL4HJK2","target":"record","payload":{"canonical_record":{"source":{"id":"2407.11206","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-07-15T19:41:00Z","cross_cats_sorted":[],"title_canon_sha256":"536ef8f106ae4a293ed375d62f739534323fdf99d9b8bf450ff1fb84519c3985","abstract_canon_sha256":"f3589c0114a273458ab2c81c96edfe9084685e4253954eb4bdc1a8df5cedbdaf"},"schema_version":"1.0"},"canonical_sha256":"1d26f4b8be62a89693a5804c15f0e956a1b8f80f29e441f0a01b0ba1f3c0af99","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:18:39.608042Z","signature_b64":"DNNamTR7WXqXXi+/vIjSzNm7ZdfqcACrGyFtl1C8m85oNjg/61A8IJvOg7+gmNffe1v/B5HFFdmOPWJjU+RcCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1d26f4b8be62a89693a5804c15f0e956a1b8f80f29e441f0a01b0ba1f3c0af99","last_reissued_at":"2026-07-05T10:18:39.607490Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:18:39.607490Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2407.11206","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T10:18:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ADBB5FwA1rbkBxmuSuEYJ5rzeiut/VtphVqD+9mEEYRYQ8l0S5DH6j1UnMVBOe8priHRF9xq3DKlY61DTYvKAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-07T05:57:00.903804Z"},"content_sha256":"fc7acf60f78dea28f0dff197c4995c5b1d939e14809cec95495b22b05bb94cf5","schema_version":"1.0","event_id":"sha256:fc7acf60f78dea28f0dff197c4995c5b1d939e14809cec95495b22b05bb94cf5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:DUTPJOF6MKUJNE5FQBGBL4HJK2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Deep flows transmitted by forced surface gravity waves","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Gregory L. Wagner, Nick Pizzo","submitted_at":"2024-07-15T19:41:00Z","abstract_excerpt":"We examine a two-dimensional deep-water surface gravity wave packet generated by a pressure disturbance in the Lagrangian reference frame. The pressure disturbance has the form of a narrow-banded weakly nonlinear deep-water wave packet. During forcing, the vorticity equation implies that the momentum resides entirely in the near-surface Lagrangian-mean flow, which in this context is often called the ``Stokes drift''. After the forcing turns off, the wave packet propagates away from the forcing region, carrying with it most of the energy imparted by the forcing. These waves together with their "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2407.11206","kind":"arxiv","version":2},"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/2407.11206/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T10:18:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"44c3o2rC1hz4TUjDHOKAQDa9X5LjaYrs2QZwGUgwAlPKrNgtW0TC+ZDRrR1bNw77ie59NM3gGuf82xnzDaU+AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-07T05:57:00.904456Z"},"content_sha256":"a750d693c35fbae10b75be985845b159cc4775cff30ac6132914ac2042aea004","schema_version":"1.0","event_id":"sha256:a750d693c35fbae10b75be985845b159cc4775cff30ac6132914ac2042aea004"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DUTPJOF6MKUJNE5FQBGBL4HJK2/bundle.json","state_url":"https://pith.science/pith/DUTPJOF6MKUJNE5FQBGBL4HJK2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DUTPJOF6MKUJNE5FQBGBL4HJK2/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-07-07T05:57:00Z","links":{"resolver":"https://pith.science/pith/DUTPJOF6MKUJNE5FQBGBL4HJK2","bundle":"https://pith.science/pith/DUTPJOF6MKUJNE5FQBGBL4HJK2/bundle.json","state":"https://pith.science/pith/DUTPJOF6MKUJNE5FQBGBL4HJK2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DUTPJOF6MKUJNE5FQBGBL4HJK2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:DUTPJOF6MKUJNE5FQBGBL4HJK2","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":"f3589c0114a273458ab2c81c96edfe9084685e4253954eb4bdc1a8df5cedbdaf","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-07-15T19:41:00Z","title_canon_sha256":"536ef8f106ae4a293ed375d62f739534323fdf99d9b8bf450ff1fb84519c3985"},"schema_version":"1.0","source":{"id":"2407.11206","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2407.11206","created_at":"2026-07-05T10:18:39Z"},{"alias_kind":"arxiv_version","alias_value":"2407.11206v2","created_at":"2026-07-05T10:18:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2407.11206","created_at":"2026-07-05T10:18:39Z"},{"alias_kind":"pith_short_12","alias_value":"DUTPJOF6MKUJ","created_at":"2026-07-05T10:18:39Z"},{"alias_kind":"pith_short_16","alias_value":"DUTPJOF6MKUJNE5F","created_at":"2026-07-05T10:18:39Z"},{"alias_kind":"pith_short_8","alias_value":"DUTPJOF6","created_at":"2026-07-05T10:18:39Z"}],"graph_snapshots":[{"event_id":"sha256:a750d693c35fbae10b75be985845b159cc4775cff30ac6132914ac2042aea004","target":"graph","created_at":"2026-07-05T10:18:39Z","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/2407.11206/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We examine a two-dimensional deep-water surface gravity wave packet generated by a pressure disturbance in the Lagrangian reference frame. The pressure disturbance has the form of a narrow-banded weakly nonlinear deep-water wave packet. During forcing, the vorticity equation implies that the momentum resides entirely in the near-surface Lagrangian-mean flow, which in this context is often called the ``Stokes drift''. After the forcing turns off, the wave packet propagates away from the forcing region, carrying with it most of the energy imparted by the forcing. These waves together with their ","authors_text":"Gregory L. Wagner, Nick Pizzo","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-07-15T19:41:00Z","title":"Deep flows transmitted by forced surface gravity waves"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2407.11206","kind":"arxiv","version":2},"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:fc7acf60f78dea28f0dff197c4995c5b1d939e14809cec95495b22b05bb94cf5","target":"record","created_at":"2026-07-05T10:18:39Z","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":"f3589c0114a273458ab2c81c96edfe9084685e4253954eb4bdc1a8df5cedbdaf","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-07-15T19:41:00Z","title_canon_sha256":"536ef8f106ae4a293ed375d62f739534323fdf99d9b8bf450ff1fb84519c3985"},"schema_version":"1.0","source":{"id":"2407.11206","kind":"arxiv","version":2}},"canonical_sha256":"1d26f4b8be62a89693a5804c15f0e956a1b8f80f29e441f0a01b0ba1f3c0af99","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1d26f4b8be62a89693a5804c15f0e956a1b8f80f29e441f0a01b0ba1f3c0af99","first_computed_at":"2026-07-05T10:18:39.607490Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:18:39.607490Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DNNamTR7WXqXXi+/vIjSzNm7ZdfqcACrGyFtl1C8m85oNjg/61A8IJvOg7+gmNffe1v/B5HFFdmOPWJjU+RcCw==","signature_status":"signed_v1","signed_at":"2026-07-05T10:18:39.608042Z","signed_message":"canonical_sha256_bytes"},"source_id":"2407.11206","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fc7acf60f78dea28f0dff197c4995c5b1d939e14809cec95495b22b05bb94cf5","sha256:a750d693c35fbae10b75be985845b159cc4775cff30ac6132914ac2042aea004"],"state_sha256":"ef9aa92569cd047598eb3acf4354008cbca593944a2774f70e099924ae2cbc42"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"enVGecjQHIiXX7C0hZXwMzcs5YNZltgzkQBa0oc9maQNoUpDtXKE+Pp92c3RPhO5i67Ky65LjhsYvFl9Bk26Dw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-07T05:57:00.907599Z","bundle_sha256":"86a61298829fba51722428f8266058df969195a530eed43cb9534a388e38d8a2"}}