{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:VISHQTPW5ITWF54QVWW2W7YKPP","short_pith_number":"pith:VISHQTPW","canonical_record":{"source":{"id":"1702.08468","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-02-27T19:01:36Z","cross_cats_sorted":[],"title_canon_sha256":"8dcabbc8cc451d193330c9e621eea42e0476c01879c66a1c29aea7d840ac975d","abstract_canon_sha256":"6ed7e72647ebf6bbba24ea74497aec90c22277edc086762ea5383e9c1de7d23f"},"schema_version":"1.0"},"canonical_sha256":"aa24784df6ea2762f790adadab7f0a7bc2d5757f430d1eca0cf4214cc7935e2c","source":{"kind":"arxiv","id":"1702.08468","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.08468","created_at":"2026-05-18T00:38:57Z"},{"alias_kind":"arxiv_version","alias_value":"1702.08468v1","created_at":"2026-05-18T00:38:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.08468","created_at":"2026-05-18T00:38:57Z"},{"alias_kind":"pith_short_12","alias_value":"VISHQTPW5ITW","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"VISHQTPW5ITWF54Q","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"VISHQTPW","created_at":"2026-05-18T12:31:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:VISHQTPW5ITWF54QVWW2W7YKPP","target":"record","payload":{"canonical_record":{"source":{"id":"1702.08468","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-02-27T19:01:36Z","cross_cats_sorted":[],"title_canon_sha256":"8dcabbc8cc451d193330c9e621eea42e0476c01879c66a1c29aea7d840ac975d","abstract_canon_sha256":"6ed7e72647ebf6bbba24ea74497aec90c22277edc086762ea5383e9c1de7d23f"},"schema_version":"1.0"},"canonical_sha256":"aa24784df6ea2762f790adadab7f0a7bc2d5757f430d1eca0cf4214cc7935e2c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:57.255524Z","signature_b64":"vQEd5X8j8ZRBv1Kuo31t13SWSpR9psfGW3DCwGnZXxwqGdr/jl6FwyDpLpWMx+EypSVTv+cEk8g1aAQXhN76Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aa24784df6ea2762f790adadab7f0a7bc2d5757f430d1eca0cf4214cc7935e2c","last_reissued_at":"2026-05-18T00:38:57.254992Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:57.254992Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1702.08468","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:38:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fG0am3lHVP3mj1/wqFl+A8lljtqLmj1hAnzIDmIOiGV1vYSifvUxlSOJX9B156/cLlp7sXfJBSEERN+xaf8PAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T21:37:25.098054Z"},"content_sha256":"cca171e65ad69c781c7b8f7857b436edcc386fb250df36991f30c469eac62aec","schema_version":"1.0","event_id":"sha256:cca171e65ad69c781c7b8f7857b436edcc386fb250df36991f30c469eac62aec"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:VISHQTPW5ITWF54QVWW2W7YKPP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Emergence of Multi-Scaling in a Random Force-Stirred Fluid","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Diego Donzis, Victor Yakhot","submitted_at":"2017-02-27T19:01:36Z","abstract_excerpt":"We consider transition to strong turbulence in an infinite fluid stirred by a gaussian random force. The transition is {\\bf defined} as a first appearance of anomalous scaling of normalized moments of velocity derivatives (dissipation rates) emerging from the low-Reynolds-number Gaussian background. It is shown that due to multi-scaling, strongly intermittent rare events can be quantitatively described in terms of an infinite number of different \"Reynolds numbers\" reflecting multitude of anomalous scaling exponents. The theoretically predicted transition disappears at $R_{\\lambda}\\leq 3$. The "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.08468","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":""},"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":"2026-05-18T00:38:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4auiAWje29U4vRqihYR0gBDx4IOEcniMCo+vNRamgDwIdMQ2Zfaa4/zLLpSFOJ/z1fpGoaLDCbqRiVjugMqRDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T21:37:25.098409Z"},"content_sha256":"ea2cfac741e63e71f7bf9a50f0466d0d75e51bdefc7effae1ca0222edc8ec4a1","schema_version":"1.0","event_id":"sha256:ea2cfac741e63e71f7bf9a50f0466d0d75e51bdefc7effae1ca0222edc8ec4a1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VISHQTPW5ITWF54QVWW2W7YKPP/bundle.json","state_url":"https://pith.science/pith/VISHQTPW5ITWF54QVWW2W7YKPP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VISHQTPW5ITWF54QVWW2W7YKPP/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":"2026-06-02T21:37:25Z","links":{"resolver":"https://pith.science/pith/VISHQTPW5ITWF54QVWW2W7YKPP","bundle":"https://pith.science/pith/VISHQTPW5ITWF54QVWW2W7YKPP/bundle.json","state":"https://pith.science/pith/VISHQTPW5ITWF54QVWW2W7YKPP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VISHQTPW5ITWF54QVWW2W7YKPP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:VISHQTPW5ITWF54QVWW2W7YKPP","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":"6ed7e72647ebf6bbba24ea74497aec90c22277edc086762ea5383e9c1de7d23f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-02-27T19:01:36Z","title_canon_sha256":"8dcabbc8cc451d193330c9e621eea42e0476c01879c66a1c29aea7d840ac975d"},"schema_version":"1.0","source":{"id":"1702.08468","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.08468","created_at":"2026-05-18T00:38:57Z"},{"alias_kind":"arxiv_version","alias_value":"1702.08468v1","created_at":"2026-05-18T00:38:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.08468","created_at":"2026-05-18T00:38:57Z"},{"alias_kind":"pith_short_12","alias_value":"VISHQTPW5ITW","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"VISHQTPW5ITWF54Q","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"VISHQTPW","created_at":"2026-05-18T12:31:49Z"}],"graph_snapshots":[{"event_id":"sha256:ea2cfac741e63e71f7bf9a50f0466d0d75e51bdefc7effae1ca0222edc8ec4a1","target":"graph","created_at":"2026-05-18T00:38:57Z","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":"We consider transition to strong turbulence in an infinite fluid stirred by a gaussian random force. The transition is {\\bf defined} as a first appearance of anomalous scaling of normalized moments of velocity derivatives (dissipation rates) emerging from the low-Reynolds-number Gaussian background. It is shown that due to multi-scaling, strongly intermittent rare events can be quantitatively described in terms of an infinite number of different \"Reynolds numbers\" reflecting multitude of anomalous scaling exponents. The theoretically predicted transition disappears at $R_{\\lambda}\\leq 3$. The ","authors_text":"Diego Donzis, Victor Yakhot","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-02-27T19:01:36Z","title":"Emergence of Multi-Scaling in a Random Force-Stirred Fluid"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.08468","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:cca171e65ad69c781c7b8f7857b436edcc386fb250df36991f30c469eac62aec","target":"record","created_at":"2026-05-18T00:38:57Z","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":"6ed7e72647ebf6bbba24ea74497aec90c22277edc086762ea5383e9c1de7d23f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-02-27T19:01:36Z","title_canon_sha256":"8dcabbc8cc451d193330c9e621eea42e0476c01879c66a1c29aea7d840ac975d"},"schema_version":"1.0","source":{"id":"1702.08468","kind":"arxiv","version":1}},"canonical_sha256":"aa24784df6ea2762f790adadab7f0a7bc2d5757f430d1eca0cf4214cc7935e2c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aa24784df6ea2762f790adadab7f0a7bc2d5757f430d1eca0cf4214cc7935e2c","first_computed_at":"2026-05-18T00:38:57.254992Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:38:57.254992Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vQEd5X8j8ZRBv1Kuo31t13SWSpR9psfGW3DCwGnZXxwqGdr/jl6FwyDpLpWMx+EypSVTv+cEk8g1aAQXhN76Aw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:38:57.255524Z","signed_message":"canonical_sha256_bytes"},"source_id":"1702.08468","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cca171e65ad69c781c7b8f7857b436edcc386fb250df36991f30c469eac62aec","sha256:ea2cfac741e63e71f7bf9a50f0466d0d75e51bdefc7effae1ca0222edc8ec4a1"],"state_sha256":"883ea251e65ddd32ba5f5bd2301b4670d7a64a140c53af847ed99916bbbcb848"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4SdUK10UwRQitw/VK+tDFkHGoMmf7XXovZAwYsGTfCbCz1NayydKsXtad5StgoSVgR3mjv2C+vkTL6F0mVGlAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T21:37:25.100329Z","bundle_sha256":"0352ad6ff38c45725ef139d3d2044483d828d4e5bd958396c76cb245b38119e8"}}