{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:BCSX6NTBB3W62MRGIQPIR3EA2A","short_pith_number":"pith:BCSX6NTB","canonical_record":{"source":{"id":"1712.05333","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-12-14T17:00:11Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"7d10fc5e18bc79045dc656bb1f78a91269b1d78a78a893b141d92302c9f7286b","abstract_canon_sha256":"eda05b3379a0f2618e80d54501325b4e381e6095082a86c5c20238f6093f4d42"},"schema_version":"1.0"},"canonical_sha256":"08a57f36610eeded3226441e88ec80d03a6d433c05a4538b86ae0f328ce2f1be","source":{"kind":"arxiv","id":"1712.05333","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1712.05333","created_at":"2026-05-18T00:27:58Z"},{"alias_kind":"arxiv_version","alias_value":"1712.05333v1","created_at":"2026-05-18T00:27:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.05333","created_at":"2026-05-18T00:27:58Z"},{"alias_kind":"pith_short_12","alias_value":"BCSX6NTBB3W6","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"BCSX6NTBB3W62MRG","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"BCSX6NTB","created_at":"2026-05-18T12:31:08Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:BCSX6NTBB3W62MRGIQPIR3EA2A","target":"record","payload":{"canonical_record":{"source":{"id":"1712.05333","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-12-14T17:00:11Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"7d10fc5e18bc79045dc656bb1f78a91269b1d78a78a893b141d92302c9f7286b","abstract_canon_sha256":"eda05b3379a0f2618e80d54501325b4e381e6095082a86c5c20238f6093f4d42"},"schema_version":"1.0"},"canonical_sha256":"08a57f36610eeded3226441e88ec80d03a6d433c05a4538b86ae0f328ce2f1be","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:27:58.183965Z","signature_b64":"4lsDy82iqt6SDW4XHmbhoTL0vr6FeHxavx6O97abjYNvTCZnmit+AAatvxG15qotxobrmyobfBr1OCzT3AL4Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"08a57f36610eeded3226441e88ec80d03a6d433c05a4538b86ae0f328ce2f1be","last_reissued_at":"2026-05-18T00:27:58.183270Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:27:58.183270Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1712.05333","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":"2026-05-18T00:27:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4a/ElNmLjTppkmm2moWekWmKd3F/XZvynLhG0nmXZuRQ6KMOhpjYwlYSnKa40bkBJfBy5LFTkIrXQkKEDWvpCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-02T07:03:27.370642Z"},"content_sha256":"4c7e4b44d2637d99234565bb2e25cabb979092aabcc59b71f3d739154c38f4ea","schema_version":"1.0","event_id":"sha256:4c7e4b44d2637d99234565bb2e25cabb979092aabcc59b71f3d739154c38f4ea"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:BCSX6NTBB3W62MRGIQPIR3EA2A","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the generation of drift flows in wall-bounded flows transiting to turbulence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.PS"],"primary_cat":"physics.flu-dyn","authors_text":"Paul Manneville","submitted_at":"2017-12-14T17:00:11Z","abstract_excerpt":"Despite recent progress, laminar-turbulent coexistence in transitional planar wall-bounded shear flows is still not well understood. Contrasting with the processes by which chaotic flow inside turbulent patches is sustained at the local (minimal flow unit) scale, the mechanisms controlling the obliqueness of laminar-turbulent interfaces typically observed all along the coexistence range are still mysterious. An extension of Waleffe's approach [Phys. Fluids 9 (1997) 883--900] is used to show that, already at the local scale, drift flows breaking the problem's spanwise symmetry are generated jus"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.05333","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":"2026-05-18T00:27:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lO54kdTh+2vVqXh2kjpiFMcDUtgcmvwpt5X9JdDhmER+vyt3yypN/fhpeu+H61joEJFbU2xNZeBeynCa+CvCDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-02T07:03:27.370989Z"},"content_sha256":"aa82f894daafcc008f54d317b0b8088a48278365fe45779538d3bf2af614b35d","schema_version":"1.0","event_id":"sha256:aa82f894daafcc008f54d317b0b8088a48278365fe45779538d3bf2af614b35d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BCSX6NTBB3W62MRGIQPIR3EA2A/bundle.json","state_url":"https://pith.science/pith/BCSX6NTBB3W62MRGIQPIR3EA2A/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BCSX6NTBB3W62MRGIQPIR3EA2A/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":"2026-07-02T07:03:27Z","links":{"resolver":"https://pith.science/pith/BCSX6NTBB3W62MRGIQPIR3EA2A","bundle":"https://pith.science/pith/BCSX6NTBB3W62MRGIQPIR3EA2A/bundle.json","state":"https://pith.science/pith/BCSX6NTBB3W62MRGIQPIR3EA2A/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BCSX6NTBB3W62MRGIQPIR3EA2A/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:BCSX6NTBB3W62MRGIQPIR3EA2A","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":"eda05b3379a0f2618e80d54501325b4e381e6095082a86c5c20238f6093f4d42","cross_cats_sorted":["nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-12-14T17:00:11Z","title_canon_sha256":"7d10fc5e18bc79045dc656bb1f78a91269b1d78a78a893b141d92302c9f7286b"},"schema_version":"1.0","source":{"id":"1712.05333","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1712.05333","created_at":"2026-05-18T00:27:58Z"},{"alias_kind":"arxiv_version","alias_value":"1712.05333v1","created_at":"2026-05-18T00:27:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.05333","created_at":"2026-05-18T00:27:58Z"},{"alias_kind":"pith_short_12","alias_value":"BCSX6NTBB3W6","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"BCSX6NTBB3W62MRG","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"BCSX6NTB","created_at":"2026-05-18T12:31:08Z"}],"graph_snapshots":[{"event_id":"sha256:aa82f894daafcc008f54d317b0b8088a48278365fe45779538d3bf2af614b35d","target":"graph","created_at":"2026-05-18T00:27:58Z","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":"Despite recent progress, laminar-turbulent coexistence in transitional planar wall-bounded shear flows is still not well understood. Contrasting with the processes by which chaotic flow inside turbulent patches is sustained at the local (minimal flow unit) scale, the mechanisms controlling the obliqueness of laminar-turbulent interfaces typically observed all along the coexistence range are still mysterious. An extension of Waleffe's approach [Phys. Fluids 9 (1997) 883--900] is used to show that, already at the local scale, drift flows breaking the problem's spanwise symmetry are generated jus","authors_text":"Paul Manneville","cross_cats":["nlin.PS"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-12-14T17:00:11Z","title":"On the generation of drift flows in wall-bounded flows transiting to turbulence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.05333","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":"sha256:4c7e4b44d2637d99234565bb2e25cabb979092aabcc59b71f3d739154c38f4ea","target":"record","created_at":"2026-05-18T00:27:58Z","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":"eda05b3379a0f2618e80d54501325b4e381e6095082a86c5c20238f6093f4d42","cross_cats_sorted":["nlin.PS"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-12-14T17:00:11Z","title_canon_sha256":"7d10fc5e18bc79045dc656bb1f78a91269b1d78a78a893b141d92302c9f7286b"},"schema_version":"1.0","source":{"id":"1712.05333","kind":"arxiv","version":1}},"canonical_sha256":"08a57f36610eeded3226441e88ec80d03a6d433c05a4538b86ae0f328ce2f1be","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"08a57f36610eeded3226441e88ec80d03a6d433c05a4538b86ae0f328ce2f1be","first_computed_at":"2026-05-18T00:27:58.183270Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:27:58.183270Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4lsDy82iqt6SDW4XHmbhoTL0vr6FeHxavx6O97abjYNvTCZnmit+AAatvxG15qotxobrmyobfBr1OCzT3AL4Dg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:27:58.183965Z","signed_message":"canonical_sha256_bytes"},"source_id":"1712.05333","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4c7e4b44d2637d99234565bb2e25cabb979092aabcc59b71f3d739154c38f4ea","sha256:aa82f894daafcc008f54d317b0b8088a48278365fe45779538d3bf2af614b35d"],"state_sha256":"2d592aebe0d9288d71fd866cd19dda9be8fd658570885e6a07a62bd36cea3e23"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CiuzwMw7+waqOX1mOTzzDEUxxemuaWotC+lLYfgxTFBQisrx2me6cnqHBBPaVWBHOjrC3T+kkrm/EwFf/ZajBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-02T07:03:27.373115Z","bundle_sha256":"9fb8fe350238f85d3eaf1c6cc1a721c0020fe5d8024007afcd2cae01619f38fd"}}