{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:BSKMZWVRYKZRUGHARZJL6DATOM","short_pith_number":"pith:BSKMZWVR","canonical_record":{"source":{"id":"1709.00823","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-09-04T06:08:14Z","cross_cats_sorted":[],"title_canon_sha256":"6a306c201312aa8ecb74137fe76158d10b4b5d57bd7c1f68833d87d47afb39aa","abstract_canon_sha256":"d017898ed19fcc57dd7750764c210e58de121c4c79e1d99631944b5bcbe7a2a5"},"schema_version":"1.0"},"canonical_sha256":"0c94ccdab1c2b31a18e08e52bf0c13731a8c2a65a0feb469ef8e224f1eb22dbb","source":{"kind":"arxiv","id":"1709.00823","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.00823","created_at":"2026-05-18T00:36:05Z"},{"alias_kind":"arxiv_version","alias_value":"1709.00823v1","created_at":"2026-05-18T00:36:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.00823","created_at":"2026-05-18T00:36:05Z"},{"alias_kind":"pith_short_12","alias_value":"BSKMZWVRYKZR","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"BSKMZWVRYKZRUGHA","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"BSKMZWVR","created_at":"2026-05-18T12:31:08Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:BSKMZWVRYKZRUGHARZJL6DATOM","target":"record","payload":{"canonical_record":{"source":{"id":"1709.00823","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-09-04T06:08:14Z","cross_cats_sorted":[],"title_canon_sha256":"6a306c201312aa8ecb74137fe76158d10b4b5d57bd7c1f68833d87d47afb39aa","abstract_canon_sha256":"d017898ed19fcc57dd7750764c210e58de121c4c79e1d99631944b5bcbe7a2a5"},"schema_version":"1.0"},"canonical_sha256":"0c94ccdab1c2b31a18e08e52bf0c13731a8c2a65a0feb469ef8e224f1eb22dbb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:36:05.036294Z","signature_b64":"dpg8P3nvDYHem5NF5L0l0DAoEEjLQqYN9lTYJVLSmfjPOpd70uL/G+TFKdiiMD++0UOEhd2FfpuRdqcPLFt8BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0c94ccdab1c2b31a18e08e52bf0c13731a8c2a65a0feb469ef8e224f1eb22dbb","last_reissued_at":"2026-05-18T00:36:05.035811Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:36:05.035811Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1709.00823","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":"2026-05-18T00:36:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0Cj0laob0i2ii8ONeiR/xsRIlw53nqE/cRnA1FttdpjlEV5Ejt+2Agz5KNTTKc7thyhTFGAhX5gJWCRD0MwUDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T02:12:00.000424Z"},"content_sha256":"c1ac21ea6a761f56753011f710ae3a69dcd47158a17020e3a307d9d5065fb7fc","schema_version":"1.0","event_id":"sha256:c1ac21ea6a761f56753011f710ae3a69dcd47158a17020e3a307d9d5065fb7fc"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:BSKMZWVRYKZRUGHARZJL6DATOM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Multiscale analysis of the topological invariants in the logarithmic region of turbulent channels at $Re_{\\tau}=932$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Adri\\'an Lozano-Dur\\'an, Javier Jim\\'enez, Markus Holzner","submitted_at":"2017-09-04T06:08:14Z","abstract_excerpt":"The invariants of the velocity gradient tensor, $R$ and $Q$, and their enstrophy and strain components are studied in the logarithmic layer of an incompressible turbulent channel flow. The velocities are filtered in the three spatial directions and the results analyzed at different scales. We show that the $R$--$Q$ plane does not capture the changes undergone by the flow as the filter width increases, and that the enstrophy/enstrophy-production and strain/strain-production planes represent better choices. We also show that the conditional mean trajectories may differ significantly from the ins"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.00823","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":"2026-05-18T00:36:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7USbF8C7lnnSbqjhiTR1w2kqFqpTJvDIEeCBTonjVi0UqQm36D3a3lon8zEl50gYKHHvdL5EOJX6PZN8gRGCBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T02:12:00.000996Z"},"content_sha256":"249f203b1c7ce1d7f269a87ec625b5ef300e43c2ec3a9fa483026cf15aa32bd3","schema_version":"1.0","event_id":"sha256:249f203b1c7ce1d7f269a87ec625b5ef300e43c2ec3a9fa483026cf15aa32bd3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BSKMZWVRYKZRUGHARZJL6DATOM/bundle.json","state_url":"https://pith.science/pith/BSKMZWVRYKZRUGHARZJL6DATOM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BSKMZWVRYKZRUGHARZJL6DATOM/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":"2026-05-31T02:12:00Z","links":{"resolver":"https://pith.science/pith/BSKMZWVRYKZRUGHARZJL6DATOM","bundle":"https://pith.science/pith/BSKMZWVRYKZRUGHARZJL6DATOM/bundle.json","state":"https://pith.science/pith/BSKMZWVRYKZRUGHARZJL6DATOM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BSKMZWVRYKZRUGHARZJL6DATOM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:BSKMZWVRYKZRUGHARZJL6DATOM","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":"d017898ed19fcc57dd7750764c210e58de121c4c79e1d99631944b5bcbe7a2a5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-09-04T06:08:14Z","title_canon_sha256":"6a306c201312aa8ecb74137fe76158d10b4b5d57bd7c1f68833d87d47afb39aa"},"schema_version":"1.0","source":{"id":"1709.00823","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.00823","created_at":"2026-05-18T00:36:05Z"},{"alias_kind":"arxiv_version","alias_value":"1709.00823v1","created_at":"2026-05-18T00:36:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.00823","created_at":"2026-05-18T00:36:05Z"},{"alias_kind":"pith_short_12","alias_value":"BSKMZWVRYKZR","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"BSKMZWVRYKZRUGHA","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"BSKMZWVR","created_at":"2026-05-18T12:31:08Z"}],"graph_snapshots":[{"event_id":"sha256:249f203b1c7ce1d7f269a87ec625b5ef300e43c2ec3a9fa483026cf15aa32bd3","target":"graph","created_at":"2026-05-18T00:36:05Z","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":"The invariants of the velocity gradient tensor, $R$ and $Q$, and their enstrophy and strain components are studied in the logarithmic layer of an incompressible turbulent channel flow. The velocities are filtered in the three spatial directions and the results analyzed at different scales. We show that the $R$--$Q$ plane does not capture the changes undergone by the flow as the filter width increases, and that the enstrophy/enstrophy-production and strain/strain-production planes represent better choices. We also show that the conditional mean trajectories may differ significantly from the ins","authors_text":"Adri\\'an Lozano-Dur\\'an, Javier Jim\\'enez, Markus Holzner","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-09-04T06:08:14Z","title":"Multiscale analysis of the topological invariants in the logarithmic region of turbulent channels at $Re_{\\tau}=932$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.00823","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:c1ac21ea6a761f56753011f710ae3a69dcd47158a17020e3a307d9d5065fb7fc","target":"record","created_at":"2026-05-18T00:36:05Z","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":"d017898ed19fcc57dd7750764c210e58de121c4c79e1d99631944b5bcbe7a2a5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-09-04T06:08:14Z","title_canon_sha256":"6a306c201312aa8ecb74137fe76158d10b4b5d57bd7c1f68833d87d47afb39aa"},"schema_version":"1.0","source":{"id":"1709.00823","kind":"arxiv","version":1}},"canonical_sha256":"0c94ccdab1c2b31a18e08e52bf0c13731a8c2a65a0feb469ef8e224f1eb22dbb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0c94ccdab1c2b31a18e08e52bf0c13731a8c2a65a0feb469ef8e224f1eb22dbb","first_computed_at":"2026-05-18T00:36:05.035811Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:36:05.035811Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"dpg8P3nvDYHem5NF5L0l0DAoEEjLQqYN9lTYJVLSmfjPOpd70uL/G+TFKdiiMD++0UOEhd2FfpuRdqcPLFt8BQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:36:05.036294Z","signed_message":"canonical_sha256_bytes"},"source_id":"1709.00823","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c1ac21ea6a761f56753011f710ae3a69dcd47158a17020e3a307d9d5065fb7fc","sha256:249f203b1c7ce1d7f269a87ec625b5ef300e43c2ec3a9fa483026cf15aa32bd3"],"state_sha256":"048ac20b61c849bb1c9bd490c9993d6ca2bab3f040100400add2b13f67277acf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mQPRBe0pfd/dGMnl2tYxv2ZeDQXQ4Oi80XjRz66liCj9U1cb+M8NRr/t3U45gnVju6J+JMrVmG9lGbI+H+tZBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T02:12:00.003162Z","bundle_sha256":"0febe9abe532e359f9bcb84145f413bb6bd6d76e60d21a6a28e2dc8c81c5bf38"}}