{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:C62NT3RBWJKLQBACM572QA7NBL","short_pith_number":"pith:C62NT3RB","canonical_record":{"source":{"id":"1801.06102","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2018-01-17T17:17:46Z","cross_cats_sorted":["cond-mat.stat-mech","hep-th"],"title_canon_sha256":"c51dc09a89156b7ebaa24c5e788842e79b9147021acf57beb1e5908445e13c18","abstract_canon_sha256":"49bef840f685570c652d566103112cbdeceac146eff315e4ca9c3c9ed057e164"},"schema_version":"1.0"},"canonical_sha256":"17b4d9ee21b254b80402677fa803ed0ac7762e3fb2e775061780422fe79357fe","source":{"kind":"arxiv","id":"1801.06102","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.06102","created_at":"2026-05-17T23:44:59Z"},{"alias_kind":"arxiv_version","alias_value":"1801.06102v2","created_at":"2026-05-17T23:44:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.06102","created_at":"2026-05-17T23:44:59Z"},{"alias_kind":"pith_short_12","alias_value":"C62NT3RBWJKL","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_16","alias_value":"C62NT3RBWJKLQBAC","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_8","alias_value":"C62NT3RB","created_at":"2026-05-18T12:32:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:C62NT3RBWJKLQBACM572QA7NBL","target":"record","payload":{"canonical_record":{"source":{"id":"1801.06102","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2018-01-17T17:17:46Z","cross_cats_sorted":["cond-mat.stat-mech","hep-th"],"title_canon_sha256":"c51dc09a89156b7ebaa24c5e788842e79b9147021acf57beb1e5908445e13c18","abstract_canon_sha256":"49bef840f685570c652d566103112cbdeceac146eff315e4ca9c3c9ed057e164"},"schema_version":"1.0"},"canonical_sha256":"17b4d9ee21b254b80402677fa803ed0ac7762e3fb2e775061780422fe79357fe","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:44:59.864662Z","signature_b64":"mp5PjxhFLAIZuvak3dcEggVENhdyxAiEluGskYT31xKYf2XSuwba8IdIA+A/3f9GoDXznJWCjWD/zKYwS0laBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"17b4d9ee21b254b80402677fa803ed0ac7762e3fb2e775061780422fe79357fe","last_reissued_at":"2026-05-17T23:44:59.864067Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:44:59.864067Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1801.06102","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":"2026-05-17T23:44:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yOXWvM3L+dD9DyXQbZuCdUTgjbZdv/bIwZIuVwHdFEaVxc+WJ6nlV5y699TtajloG+srY0k3wlGswCVJnG6EAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T21:40:34.078076Z"},"content_sha256":"c5368800e56d1d24b1faa4cc405dbac668fa1726d78193e484ac7d207babcc13","schema_version":"1.0","event_id":"sha256:c5368800e56d1d24b1faa4cc405dbac668fa1726d78193e484ac7d207babcc13"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:C62NT3RBWJKLQBACM572QA7NBL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Anomalous Exponents in Strong Turbulence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","hep-th"],"primary_cat":"physics.flu-dyn","authors_text":"Diego A. Donzis, Victor Yakhot","submitted_at":"2018-01-17T17:17:46Z","abstract_excerpt":"To characterize fluctuations in a turbulent flow, one usually studies different moments of velocity increments and dissipation rate, $\\overline{(v(x+r)-v(x))^{n}}\\propto r^{\\zeta_{n}}$ and $\\overline{{\\cal E}^{n}}\\propto Re^{d_{n}}$, respectively. In high Reynolds number flows, the moments of different orders cannot be simply related to each other which is the signature of anomalous scaling, one of the most puzzling features of turbulent flows. High-order moments are related to extreme, rare events and our ability to quantitatively describe them is crucially important for meteorology, heat, ma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.06102","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":"2026-05-17T23:44:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"d81Cw5shsBHglNDyZ/8Mb/kjf8pW+PLJwN7E2mjVx3fcqOrOzNi3ZH5TuiATyfGlizewk/D0eJu7AkSGnGiFBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T21:40:34.078665Z"},"content_sha256":"f4e68d039131f21bed8a88470c877b04561bf4a134f0f69636faa1dfc767db34","schema_version":"1.0","event_id":"sha256:f4e68d039131f21bed8a88470c877b04561bf4a134f0f69636faa1dfc767db34"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/C62NT3RBWJKLQBACM572QA7NBL/bundle.json","state_url":"https://pith.science/pith/C62NT3RBWJKLQBACM572QA7NBL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/C62NT3RBWJKLQBACM572QA7NBL/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":"2026-06-02T21:40:34Z","links":{"resolver":"https://pith.science/pith/C62NT3RBWJKLQBACM572QA7NBL","bundle":"https://pith.science/pith/C62NT3RBWJKLQBACM572QA7NBL/bundle.json","state":"https://pith.science/pith/C62NT3RBWJKLQBACM572QA7NBL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/C62NT3RBWJKLQBACM572QA7NBL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:C62NT3RBWJKLQBACM572QA7NBL","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":"49bef840f685570c652d566103112cbdeceac146eff315e4ca9c3c9ed057e164","cross_cats_sorted":["cond-mat.stat-mech","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2018-01-17T17:17:46Z","title_canon_sha256":"c51dc09a89156b7ebaa24c5e788842e79b9147021acf57beb1e5908445e13c18"},"schema_version":"1.0","source":{"id":"1801.06102","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.06102","created_at":"2026-05-17T23:44:59Z"},{"alias_kind":"arxiv_version","alias_value":"1801.06102v2","created_at":"2026-05-17T23:44:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.06102","created_at":"2026-05-17T23:44:59Z"},{"alias_kind":"pith_short_12","alias_value":"C62NT3RBWJKL","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_16","alias_value":"C62NT3RBWJKLQBAC","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_8","alias_value":"C62NT3RB","created_at":"2026-05-18T12:32:16Z"}],"graph_snapshots":[{"event_id":"sha256:f4e68d039131f21bed8a88470c877b04561bf4a134f0f69636faa1dfc767db34","target":"graph","created_at":"2026-05-17T23:44:59Z","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":"To characterize fluctuations in a turbulent flow, one usually studies different moments of velocity increments and dissipation rate, $\\overline{(v(x+r)-v(x))^{n}}\\propto r^{\\zeta_{n}}$ and $\\overline{{\\cal E}^{n}}\\propto Re^{d_{n}}$, respectively. In high Reynolds number flows, the moments of different orders cannot be simply related to each other which is the signature of anomalous scaling, one of the most puzzling features of turbulent flows. High-order moments are related to extreme, rare events and our ability to quantitatively describe them is crucially important for meteorology, heat, ma","authors_text":"Diego A. Donzis, Victor Yakhot","cross_cats":["cond-mat.stat-mech","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2018-01-17T17:17:46Z","title":"Anomalous Exponents in Strong Turbulence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.06102","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:c5368800e56d1d24b1faa4cc405dbac668fa1726d78193e484ac7d207babcc13","target":"record","created_at":"2026-05-17T23:44:59Z","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":"49bef840f685570c652d566103112cbdeceac146eff315e4ca9c3c9ed057e164","cross_cats_sorted":["cond-mat.stat-mech","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2018-01-17T17:17:46Z","title_canon_sha256":"c51dc09a89156b7ebaa24c5e788842e79b9147021acf57beb1e5908445e13c18"},"schema_version":"1.0","source":{"id":"1801.06102","kind":"arxiv","version":2}},"canonical_sha256":"17b4d9ee21b254b80402677fa803ed0ac7762e3fb2e775061780422fe79357fe","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"17b4d9ee21b254b80402677fa803ed0ac7762e3fb2e775061780422fe79357fe","first_computed_at":"2026-05-17T23:44:59.864067Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:44:59.864067Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mp5PjxhFLAIZuvak3dcEggVENhdyxAiEluGskYT31xKYf2XSuwba8IdIA+A/3f9GoDXznJWCjWD/zKYwS0laBA==","signature_status":"signed_v1","signed_at":"2026-05-17T23:44:59.864662Z","signed_message":"canonical_sha256_bytes"},"source_id":"1801.06102","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c5368800e56d1d24b1faa4cc405dbac668fa1726d78193e484ac7d207babcc13","sha256:f4e68d039131f21bed8a88470c877b04561bf4a134f0f69636faa1dfc767db34"],"state_sha256":"8f834154c64be0b7e54f4fb535f8b844314a0c6c297c16836653335362bb506d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JOX2SzGxKlmK1cn2HoJC/gYxDq4/btbrgrYZe8yllyn3vQVKWqHsIfZOrYHRfCCwpktig6oGEcr4xmWwg5kEAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T21:40:34.080615Z","bundle_sha256":"bbe8fc737d73fd0e1db5a893159bd7d2ce8e8ec16c8e8e86738d8442d4ecacce"}}