{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:JTQWMRXRDSFKZM6AMSBRIQVM3I","short_pith_number":"pith:JTQWMRXR","canonical_record":{"source":{"id":"1012.1725","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2010-12-08T10:07:59Z","cross_cats_sorted":["math-ph","math.MP","physics.ao-ph"],"title_canon_sha256":"8164f0ffb8f37c32c06895ea9ac0a7d67fa5a9a7d1316d2b8dd929350ecfac84","abstract_canon_sha256":"57ae2e8af6596c5c30f13e2dae870f5f12f83125eb428f99d75d168af984a4fc"},"schema_version":"1.0"},"canonical_sha256":"4ce16646f11c8aacb3c064831442acda0224a6e414e770acd6268f752e0a60a9","source":{"kind":"arxiv","id":"1012.1725","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1012.1725","created_at":"2026-05-18T04:33:51Z"},{"alias_kind":"arxiv_version","alias_value":"1012.1725v1","created_at":"2026-05-18T04:33:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1012.1725","created_at":"2026-05-18T04:33:51Z"},{"alias_kind":"pith_short_12","alias_value":"JTQWMRXRDSFK","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"JTQWMRXRDSFKZM6A","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"JTQWMRXR","created_at":"2026-05-18T12:26:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:JTQWMRXRDSFKZM6AMSBRIQVM3I","target":"record","payload":{"canonical_record":{"source":{"id":"1012.1725","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2010-12-08T10:07:59Z","cross_cats_sorted":["math-ph","math.MP","physics.ao-ph"],"title_canon_sha256":"8164f0ffb8f37c32c06895ea9ac0a7d67fa5a9a7d1316d2b8dd929350ecfac84","abstract_canon_sha256":"57ae2e8af6596c5c30f13e2dae870f5f12f83125eb428f99d75d168af984a4fc"},"schema_version":"1.0"},"canonical_sha256":"4ce16646f11c8aacb3c064831442acda0224a6e414e770acd6268f752e0a60a9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:33:51.382266Z","signature_b64":"7SHSN5Go7WbQg6Qmj5enNTPCCoygFKXoPLdz3e4WJJwQ1vT8xuYsrxK66ErHr6KgU7TgOLCoaQzaetiVqFzKBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4ce16646f11c8aacb3c064831442acda0224a6e414e770acd6268f752e0a60a9","last_reissued_at":"2026-05-18T04:33:51.381761Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:33:51.381761Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1012.1725","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":"2026-05-18T04:33:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3Ga7TmCzgRifN93fBaug+zla1OWHm1ZlVVTrFBJJF6pmbe5Gz74rHrV3OlJzpIt8OlAAWZvnz17bP8NZOUk9DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:02:17.125914Z"},"content_sha256":"bba68c873a6150581bef9a028f54406885088e0f3a17fed7eca711e9c6219b40","schema_version":"1.0","event_id":"sha256:bba68c873a6150581bef9a028f54406885088e0f3a17fed7eca711e9c6219b40"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:JTQWMRXRDSFKZM6AMSBRIQVM3I","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Experimental evidence of conformal invariance in soap film turbulent flows","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP","physics.ao-ph"],"primary_cat":"physics.flu-dyn","authors_text":"A. Pouquet, G. Artana, M.I. Auliel, P.D. Mininni, S. Thalabard","submitted_at":"2010-12-08T10:07:59Z","abstract_excerpt":"We present experimental evidence of statistical conformal invariance in isocontours of fluid thickness in experiments of two-dimensional turbulence using soap films. A Schlieren technique is used to visualize regions of the flow with constant film thickness, and association of isocontours with Schramm-L\\\"owner evolution (SLE) is used to identify conformal invariance. In experiments where an inverse energy cascade develops, statistical evidence is consistent with such an association. The diffusivity of the associated one-dimensional Brownian process is close to 8/3, a value previously identifie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1012.1725","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":"2026-05-18T04:33:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nXqc2WkkfSDH5tMBuWUoNH6ETuxPKCohd18CczvgUqXU1pZQNQ+1/ELPh6/wYWsMqnrPep88koHBa7uhYTrWCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:02:17.126614Z"},"content_sha256":"a86c176097c43cd99735bcc00589ea413feb7ef0d3e161ca7bf47e21ed428b3f","schema_version":"1.0","event_id":"sha256:a86c176097c43cd99735bcc00589ea413feb7ef0d3e161ca7bf47e21ed428b3f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JTQWMRXRDSFKZM6AMSBRIQVM3I/bundle.json","state_url":"https://pith.science/pith/JTQWMRXRDSFKZM6AMSBRIQVM3I/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JTQWMRXRDSFKZM6AMSBRIQVM3I/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":"2026-05-25T21:02:17Z","links":{"resolver":"https://pith.science/pith/JTQWMRXRDSFKZM6AMSBRIQVM3I","bundle":"https://pith.science/pith/JTQWMRXRDSFKZM6AMSBRIQVM3I/bundle.json","state":"https://pith.science/pith/JTQWMRXRDSFKZM6AMSBRIQVM3I/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JTQWMRXRDSFKZM6AMSBRIQVM3I/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:JTQWMRXRDSFKZM6AMSBRIQVM3I","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":"57ae2e8af6596c5c30f13e2dae870f5f12f83125eb428f99d75d168af984a4fc","cross_cats_sorted":["math-ph","math.MP","physics.ao-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2010-12-08T10:07:59Z","title_canon_sha256":"8164f0ffb8f37c32c06895ea9ac0a7d67fa5a9a7d1316d2b8dd929350ecfac84"},"schema_version":"1.0","source":{"id":"1012.1725","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1012.1725","created_at":"2026-05-18T04:33:51Z"},{"alias_kind":"arxiv_version","alias_value":"1012.1725v1","created_at":"2026-05-18T04:33:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1012.1725","created_at":"2026-05-18T04:33:51Z"},{"alias_kind":"pith_short_12","alias_value":"JTQWMRXRDSFK","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"JTQWMRXRDSFKZM6A","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"JTQWMRXR","created_at":"2026-05-18T12:26:09Z"}],"graph_snapshots":[{"event_id":"sha256:a86c176097c43cd99735bcc00589ea413feb7ef0d3e161ca7bf47e21ed428b3f","target":"graph","created_at":"2026-05-18T04:33:51Z","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 present experimental evidence of statistical conformal invariance in isocontours of fluid thickness in experiments of two-dimensional turbulence using soap films. A Schlieren technique is used to visualize regions of the flow with constant film thickness, and association of isocontours with Schramm-L\\\"owner evolution (SLE) is used to identify conformal invariance. In experiments where an inverse energy cascade develops, statistical evidence is consistent with such an association. The diffusivity of the associated one-dimensional Brownian process is close to 8/3, a value previously identifie","authors_text":"A. Pouquet, G. Artana, M.I. Auliel, P.D. Mininni, S. Thalabard","cross_cats":["math-ph","math.MP","physics.ao-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2010-12-08T10:07:59Z","title":"Experimental evidence of conformal invariance in soap film turbulent flows"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1012.1725","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:bba68c873a6150581bef9a028f54406885088e0f3a17fed7eca711e9c6219b40","target":"record","created_at":"2026-05-18T04:33:51Z","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":"57ae2e8af6596c5c30f13e2dae870f5f12f83125eb428f99d75d168af984a4fc","cross_cats_sorted":["math-ph","math.MP","physics.ao-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2010-12-08T10:07:59Z","title_canon_sha256":"8164f0ffb8f37c32c06895ea9ac0a7d67fa5a9a7d1316d2b8dd929350ecfac84"},"schema_version":"1.0","source":{"id":"1012.1725","kind":"arxiv","version":1}},"canonical_sha256":"4ce16646f11c8aacb3c064831442acda0224a6e414e770acd6268f752e0a60a9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4ce16646f11c8aacb3c064831442acda0224a6e414e770acd6268f752e0a60a9","first_computed_at":"2026-05-18T04:33:51.381761Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:33:51.381761Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7SHSN5Go7WbQg6Qmj5enNTPCCoygFKXoPLdz3e4WJJwQ1vT8xuYsrxK66ErHr6KgU7TgOLCoaQzaetiVqFzKBA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:33:51.382266Z","signed_message":"canonical_sha256_bytes"},"source_id":"1012.1725","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bba68c873a6150581bef9a028f54406885088e0f3a17fed7eca711e9c6219b40","sha256:a86c176097c43cd99735bcc00589ea413feb7ef0d3e161ca7bf47e21ed428b3f"],"state_sha256":"9d0bb87e7ade93337cb2b5b95ba64250b8759d42b111a87d8c103fb5204c18fd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9hcEqXxrWP/X7gCRRgLmALZbn+hJ0y2GhmgZu/hq97XPk4o7zybiZAzEhD2b2HgcNHH0MsLrArsuKTRWGrbTCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T21:02:17.133650Z","bundle_sha256":"205205c6c2fc31162318789a186131e972f063b47db3dd4cc016a528188ffdfb"}}