{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:OPTOU3VDXNZMNPDMTE4T3PPN7L","short_pith_number":"pith:OPTOU3VD","schema_version":"1.0","canonical_sha256":"73e6ea6ea3bb72c6bc6c99393dbdedfaca8a24169ac452eb53b4b5591686613e","source":{"kind":"arxiv","id":"2505.14230","version":1},"attestation_state":"computed","paper":{"title":"Geometric and kinematic indicators of breaking inception in surface gravity waves","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Daniel G. Boettger, Michael L. Banner, Russel P. Morison Xavier Barth\\'el\\'emy, Shane R. Keating","submitted_at":"2025-05-20T11:40:26Z","abstract_excerpt":"The process of breaking in surface gravity waves can be characterized by two distinct stages. Breaking onset, defined as the first visible surface manifestation of breaking, is preceded by breaking inception, which is characterized by the initiation of an irreversible process within the crest that leads inevitably to breaking. Breaking inception diagnostics formulated using the local energetic, kinematic and geometric properties of the wave crest have recently been proposed that appear to provide generic parametric threshold estimates and may facilitate the effect of wave breaking on larger sc"},"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":"2505.14230","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2025-05-20T11:40:26Z","cross_cats_sorted":[],"title_canon_sha256":"68efee3bdfbed1ea7312236da5f18b79dbbc99b5230191e2b5baffb8cc435c47","abstract_canon_sha256":"3dfe71cee95fd23566700ad042032793d7f1ef4d0642a71cb18a0b6b004cfe1c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:05:57.999051Z","signature_b64":"O2R48DtCEOJeanKfZvwZ679oWURY1qKu6K92N0sDiafq18mUP/UP8WEmXOxkTeqxVzqOcyp7drLL8AI1GTfhAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"73e6ea6ea3bb72c6bc6c99393dbdedfaca8a24169ac452eb53b4b5591686613e","last_reissued_at":"2026-07-05T11:05:57.998573Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:05:57.998573Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Geometric and kinematic indicators of breaking inception in surface gravity waves","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Daniel G. Boettger, Michael L. Banner, Russel P. Morison Xavier Barth\\'el\\'emy, Shane R. Keating","submitted_at":"2025-05-20T11:40:26Z","abstract_excerpt":"The process of breaking in surface gravity waves can be characterized by two distinct stages. Breaking onset, defined as the first visible surface manifestation of breaking, is preceded by breaking inception, which is characterized by the initiation of an irreversible process within the crest that leads inevitably to breaking. Breaking inception diagnostics formulated using the local energetic, kinematic and geometric properties of the wave crest have recently been proposed that appear to provide generic parametric threshold estimates and may facilitate the effect of wave breaking on larger sc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.14230","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/2505.14230/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":"2505.14230","created_at":"2026-07-05T11:05:57.998635+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.14230v1","created_at":"2026-07-05T11:05:57.998635+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.14230","created_at":"2026-07-05T11:05:57.998635+00:00"},{"alias_kind":"pith_short_12","alias_value":"OPTOU3VDXNZM","created_at":"2026-07-05T11:05:57.998635+00:00"},{"alias_kind":"pith_short_16","alias_value":"OPTOU3VDXNZMNPDM","created_at":"2026-07-05T11:05:57.998635+00:00"},{"alias_kind":"pith_short_8","alias_value":"OPTOU3VD","created_at":"2026-07-05T11:05:57.998635+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/OPTOU3VDXNZMNPDMTE4T3PPN7L","json":"https://pith.science/pith/OPTOU3VDXNZMNPDMTE4T3PPN7L.json","graph_json":"https://pith.science/api/pith-number/OPTOU3VDXNZMNPDMTE4T3PPN7L/graph.json","events_json":"https://pith.science/api/pith-number/OPTOU3VDXNZMNPDMTE4T3PPN7L/events.json","paper":"https://pith.science/paper/OPTOU3VD"},"agent_actions":{"view_html":"https://pith.science/pith/OPTOU3VDXNZMNPDMTE4T3PPN7L","download_json":"https://pith.science/pith/OPTOU3VDXNZMNPDMTE4T3PPN7L.json","view_paper":"https://pith.science/paper/OPTOU3VD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.14230&json=true","fetch_graph":"https://pith.science/api/pith-number/OPTOU3VDXNZMNPDMTE4T3PPN7L/graph.json","fetch_events":"https://pith.science/api/pith-number/OPTOU3VDXNZMNPDMTE4T3PPN7L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OPTOU3VDXNZMNPDMTE4T3PPN7L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OPTOU3VDXNZMNPDMTE4T3PPN7L/action/storage_attestation","attest_author":"https://pith.science/pith/OPTOU3VDXNZMNPDMTE4T3PPN7L/action/author_attestation","sign_citation":"https://pith.science/pith/OPTOU3VDXNZMNPDMTE4T3PPN7L/action/citation_signature","submit_replication":"https://pith.science/pith/OPTOU3VDXNZMNPDMTE4T3PPN7L/action/replication_record"}},"created_at":"2026-07-05T11:05:57.998635+00:00","updated_at":"2026-07-05T11:05:57.998635+00:00"}