{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:JZFVOI5I2MOUYVTHPZPBV5WSIO","short_pith_number":"pith:JZFVOI5I","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"},"canonical_sha256":"4e4b5723a8d31d4c56677e5e1af6d243b46af41768a5d7a628f86bb35d85265d","source":{"kind":"arxiv","id":"1605.08818","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.08818","created_at":"2026-05-18T00:54:36Z"},{"alias_kind":"arxiv_version","alias_value":"1605.08818v2","created_at":"2026-05-18T00:54:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.08818","created_at":"2026-05-18T00:54:36Z"},{"alias_kind":"pith_short_12","alias_value":"JZFVOI5I2MOU","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_16","alias_value":"JZFVOI5I2MOUYVTH","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_8","alias_value":"JZFVOI5I","created_at":"2026-05-18T12:30:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:JZFVOI5I2MOUYVTHPZPBV5WSIO","target":"record","payload":{"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"},"canonical_sha256":"4e4b5723a8d31d4c56677e5e1af6d243b46af41768a5d7a628f86bb35d85265d","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"},"source_kind":"arxiv","source_id":"1605.08818","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":"2026-05-18T00:54:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gQt1pinyxxQWsXfjHpkgbd7BkfKqytjXgSQRGPfqtzjO6N1ahICIrMXf0KRbRSG8V39Cm6c9dmqHl0DRXd+wDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T13:58:54.758184Z"},"content_sha256":"ac2239cb1ad16c6b23d89d36168964b27ce93d945536f36bcce4aa8e01dc5359","schema_version":"1.0","event_id":"sha256:ac2239cb1ad16c6b23d89d36168964b27ce93d945536f36bcce4aa8e01dc5359"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:JZFVOI5I2MOUYVTHPZPBV5WSIO","target":"graph","payload":{"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:54:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"e5F5z3julPmee8W2Ts/sMEl/oqqjeAQt3K6Z6QN5ImVykg9TkY1XffFLThC9T0IWvkg1l+XIAJiPjb/hzTdHDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T13:58:54.758567Z"},"content_sha256":"302fac2ffa549712e77f4d55d828f515d4e3461dc9faae7ea3587e06097eaeca","schema_version":"1.0","event_id":"sha256:302fac2ffa549712e77f4d55d828f515d4e3461dc9faae7ea3587e06097eaeca"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO/bundle.json","state_url":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO/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":"2026-06-08T13:58:54Z","links":{"resolver":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO","bundle":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO/bundle.json","state":"https://pith.science/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JZFVOI5I2MOUYVTHPZPBV5WSIO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:JZFVOI5I2MOUYVTHPZPBV5WSIO","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":"845608b579d7b957a79abc1ed45a223ac1fe84219308f9a1517aed4e95d25b6c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2016-05-27T23:34:36Z","title_canon_sha256":"342a9aee5e9935f764ed410576d997c8eae9486137f15d77e9ee03312d1d83a5"},"schema_version":"1.0","source":{"id":"1605.08818","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.08818","created_at":"2026-05-18T00:54:36Z"},{"alias_kind":"arxiv_version","alias_value":"1605.08818v2","created_at":"2026-05-18T00:54:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.08818","created_at":"2026-05-18T00:54:36Z"},{"alias_kind":"pith_short_12","alias_value":"JZFVOI5I2MOU","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_16","alias_value":"JZFVOI5I2MOUYVTH","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_8","alias_value":"JZFVOI5I","created_at":"2026-05-18T12:30:25Z"}],"graph_snapshots":[{"event_id":"sha256:302fac2ffa549712e77f4d55d828f515d4e3461dc9faae7ea3587e06097eaeca","target":"graph","created_at":"2026-05-18T00:54:36Z","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"},"paper":{"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","authors_text":"P. Clark di Leoni, P. D. Mininni","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2016-05-27T23:34:36Z","title":"Quantifying resonant and near-resonant interactions in rotating turbulence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.08818","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:ac2239cb1ad16c6b23d89d36168964b27ce93d945536f36bcce4aa8e01dc5359","target":"record","created_at":"2026-05-18T00:54:36Z","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":"845608b579d7b957a79abc1ed45a223ac1fe84219308f9a1517aed4e95d25b6c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2016-05-27T23:34:36Z","title_canon_sha256":"342a9aee5e9935f764ed410576d997c8eae9486137f15d77e9ee03312d1d83a5"},"schema_version":"1.0","source":{"id":"1605.08818","kind":"arxiv","version":2}},"canonical_sha256":"4e4b5723a8d31d4c56677e5e1af6d243b46af41768a5d7a628f86bb35d85265d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4e4b5723a8d31d4c56677e5e1af6d243b46af41768a5d7a628f86bb35d85265d","first_computed_at":"2026-05-18T00:54:36.364384Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:54:36.364384Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zqfJa8SN0JWO+DIygNpuRBjjRjEHF02Tfrg8+wq++Pip9aFdMgdGu8xor0zpwB64jA5TTYhD3wjrUfS0FeBpAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:54:36.364976Z","signed_message":"canonical_sha256_bytes"},"source_id":"1605.08818","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ac2239cb1ad16c6b23d89d36168964b27ce93d945536f36bcce4aa8e01dc5359","sha256:302fac2ffa549712e77f4d55d828f515d4e3461dc9faae7ea3587e06097eaeca"],"state_sha256":"5e1b93e951093ac1d3a02b0be3da3638d3011bf4da2dead80b50886d0e8ddd8a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gMLSJSvb3ZHqkW5BsH/LmVXjb9LXeSO1mARDmFduhpjkG3U+AUXgNW2JP+/w7NYwxwKIwA2VZWFiJ0+hXdvtAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T13:58:54.762100Z","bundle_sha256":"fef2dc225c9fbbdc3ee0c6d981c4e9e92af97cf7525da25e9b85b752c43a52de"}}