{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:JZFVOI5I2MOUYVTHPZPBV5WSIO","short_pith_number":"pith:JZFVOI5I","schema_version":"1.0","canonical_sha256":"4e4b5723a8d31d4c56677e5e1af6d243b46af41768a5d7a628f86bb35d85265d","source":{"kind":"arxiv","id":"1605.08818","version":2},"attestation_state":"computed","paper":{"title":"Quantifying resonant and near-resonant interactions in rotating turbulence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"P. Clark di Leoni, P. D. Mininni","submitted_at":"2016-05-27T23:34:36Z","abstract_excerpt":"Nonlinear triadic interactions are at the heart of our understanding of turbulence. In flows where waves are present modes must not only be in a triad to interact, but their frequencies must also satisfy an extra condition: the interactions that dominate the energy transfer are expected to be resonant. We derive equations that allow direct measurement of the actual degree of resonance of each triad in a turbulent flow. We then apply the method to the case of rotating turbulence, where eddies coexist with inertial waves. We show that for a range of wave numbers, resonant and near-resonant triad"},"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":"1605.08818","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2016-05-27T23:34:36Z","cross_cats_sorted":[],"title_canon_sha256":"342a9aee5e9935f764ed410576d997c8eae9486137f15d77e9ee03312d1d83a5","abstract_canon_sha256":"845608b579d7b957a79abc1ed45a223ac1fe84219308f9a1517aed4e95d25b6c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:54:36.364976Z","signature_b64":"zqfJa8SN0JWO+DIygNpuRBjjRjEHF02Tfrg8+wq++Pip9aFdMgdGu8xor0zpwB64jA5TTYhD3wjrUfS0FeBpAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4e4b5723a8d31d4c56677e5e1af6d243b46af41768a5d7a628f86bb35d85265d","last_reissued_at":"2026-05-18T00:54:36.364384Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:54:36.364384Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantifying resonant and near-resonant interactions in rotating turbulence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"P. Clark di Leoni, P. D. Mininni","submitted_at":"2016-05-27T23:34:36Z","abstract_excerpt":"Nonlinear triadic interactions are at the heart of our understanding of turbulence. In flows where waves are present modes must not only be in a triad to interact, but their frequencies must also satisfy an extra condition: the interactions that dominate the energy transfer are expected to be resonant. We derive equations that allow direct measurement of the actual degree of resonance of each triad in a turbulent flow. We then apply the method to the case of rotating turbulence, where eddies coexist with inertial waves. We show that for a range of wave numbers, resonant and near-resonant triad"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.08818","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":""},"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":"1605.08818","created_at":"2026-05-18T00:54:36.364478+00:00"},{"alias_kind":"arxiv_version","alias_value":"1605.08818v2","created_at":"2026-05-18T00:54:36.364478+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.08818","created_at":"2026-05-18T00:54:36.364478+00:00"},{"alias_kind":"pith_short_12","alias_value":"JZFVOI5I2MOU","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_16","alias_value":"JZFVOI5I2MOUYVTH","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_8","alias_value":"JZFVOI5I","created_at":"2026-05-18T12:30:25.849896+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/JZFVOI5I2MOUYVTHPZPBV5WSIO","json":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO.json","graph_json":"https://pith.science/api/pith-number/JZFVOI5I2MOUYVTHPZPBV5WSIO/graph.json","events_json":"https://pith.science/api/pith-number/JZFVOI5I2MOUYVTHPZPBV5WSIO/events.json","paper":"https://pith.science/paper/JZFVOI5I"},"agent_actions":{"view_html":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO","download_json":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO.json","view_paper":"https://pith.science/paper/JZFVOI5I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1605.08818&json=true","fetch_graph":"https://pith.science/api/pith-number/JZFVOI5I2MOUYVTHPZPBV5WSIO/graph.json","fetch_events":"https://pith.science/api/pith-number/JZFVOI5I2MOUYVTHPZPBV5WSIO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO/action/storage_attestation","attest_author":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO/action/author_attestation","sign_citation":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO/action/citation_signature","submit_replication":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO/action/replication_record"}},"created_at":"2026-05-18T00:54:36.364478+00:00","updated_at":"2026-05-18T00:54:36.364478+00:00"}