{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:6KMOQPEOEKHOKSUMOF4BLSS6KT","short_pith_number":"pith:6KMOQPEO","canonical_record":{"source":{"id":"1511.07753","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2015-11-24T15:25:59Z","cross_cats_sorted":[],"title_canon_sha256":"cefa85d5c3e687c7302052286f813876d49043792ed9364fe74847f7657e3a08","abstract_canon_sha256":"6a9b884fdd4d0e56cb104a19f8df3ef837a3ba97e096a9bcc30742140286e5c4"},"schema_version":"1.0"},"canonical_sha256":"f298e83c8e228ee54a8c717815ca5e54fe9d4cdcf826d6d857fcff9ca53589a7","source":{"kind":"arxiv","id":"1511.07753","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1511.07753","created_at":"2026-05-18T01:26:03Z"},{"alias_kind":"arxiv_version","alias_value":"1511.07753v1","created_at":"2026-05-18T01:26:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.07753","created_at":"2026-05-18T01:26:03Z"},{"alias_kind":"pith_short_12","alias_value":"6KMOQPEOEKHO","created_at":"2026-05-18T12:29:07Z"},{"alias_kind":"pith_short_16","alias_value":"6KMOQPEOEKHOKSUM","created_at":"2026-05-18T12:29:07Z"},{"alias_kind":"pith_short_8","alias_value":"6KMOQPEO","created_at":"2026-05-18T12:29:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:6KMOQPEOEKHOKSUMOF4BLSS6KT","target":"record","payload":{"canonical_record":{"source":{"id":"1511.07753","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2015-11-24T15:25:59Z","cross_cats_sorted":[],"title_canon_sha256":"cefa85d5c3e687c7302052286f813876d49043792ed9364fe74847f7657e3a08","abstract_canon_sha256":"6a9b884fdd4d0e56cb104a19f8df3ef837a3ba97e096a9bcc30742140286e5c4"},"schema_version":"1.0"},"canonical_sha256":"f298e83c8e228ee54a8c717815ca5e54fe9d4cdcf826d6d857fcff9ca53589a7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:26:03.720279Z","signature_b64":"Un4it6/G4dZIvTpWooSFkjWX3fe1mVb2N9EpSNMFe2OZQa1a1SDbpylg3f3+HDc0VT9oNigyEzRO/f7NqY09AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f298e83c8e228ee54a8c717815ca5e54fe9d4cdcf826d6d857fcff9ca53589a7","last_reissued_at":"2026-05-18T01:26:03.719775Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:26:03.719775Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1511.07753","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":"2026-05-18T01:26:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XAqTS0hR6fYLhjE43Au87PU10IJR+D7r28sw3NG2oVMvFvzIQRKr2ts7am8g00ZmOT77+8lhST0aPMhuahEYBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T21:33:45.968154Z"},"content_sha256":"a6e57564d1cbf1e490530aecb7bb0b4e2e0450ff3b36b7c85f1e9c708780f66d","schema_version":"1.0","event_id":"sha256:a6e57564d1cbf1e490530aecb7bb0b4e2e0450ff3b36b7c85f1e9c708780f66d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:6KMOQPEOEKHOKSUMOF4BLSS6KT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The physics of stripe patterns in turbulent channel flow determined by DNS results","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"H. Herwig, P. Ki\\v{s}, Y. Jin","submitted_at":"2015-11-24T15:25:59Z","abstract_excerpt":"The turbulent flow in an infinitely extended plane channel is analysed by solving the Navier-Stokes equations with a DNS approach. Solutions are obtained in a numerical solution domain of finite size in the streamwise as well as in the lateral direction setting periodic boundary conditions in both directions. Their impact on large scale structures in the turbulent flow field is analysed carefully in order to avoid their suppression. When this is done appropriately well known stripe patterns in these flows can be observed and analysed especially with respect to their relative motion compared to"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.07753","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":"2026-05-18T01:26:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NW++I+ZcphNArcxufIBoEFP1zwV8+09w7PCcRXRQpMpyh6sP2+4kWuHsL4mT0UosnPH67U+WlmRtaxlL2YjIBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T21:33:45.968522Z"},"content_sha256":"f3d71aa17bcdb8fd7d9e9ae2b5e8f5be59670591588cd5b02177a351b2f256bf","schema_version":"1.0","event_id":"sha256:f3d71aa17bcdb8fd7d9e9ae2b5e8f5be59670591588cd5b02177a351b2f256bf"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6KMOQPEOEKHOKSUMOF4BLSS6KT/bundle.json","state_url":"https://pith.science/pith/6KMOQPEOEKHOKSUMOF4BLSS6KT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6KMOQPEOEKHOKSUMOF4BLSS6KT/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":"2026-06-01T21:33:45Z","links":{"resolver":"https://pith.science/pith/6KMOQPEOEKHOKSUMOF4BLSS6KT","bundle":"https://pith.science/pith/6KMOQPEOEKHOKSUMOF4BLSS6KT/bundle.json","state":"https://pith.science/pith/6KMOQPEOEKHOKSUMOF4BLSS6KT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6KMOQPEOEKHOKSUMOF4BLSS6KT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:6KMOQPEOEKHOKSUMOF4BLSS6KT","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":"6a9b884fdd4d0e56cb104a19f8df3ef837a3ba97e096a9bcc30742140286e5c4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2015-11-24T15:25:59Z","title_canon_sha256":"cefa85d5c3e687c7302052286f813876d49043792ed9364fe74847f7657e3a08"},"schema_version":"1.0","source":{"id":"1511.07753","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1511.07753","created_at":"2026-05-18T01:26:03Z"},{"alias_kind":"arxiv_version","alias_value":"1511.07753v1","created_at":"2026-05-18T01:26:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.07753","created_at":"2026-05-18T01:26:03Z"},{"alias_kind":"pith_short_12","alias_value":"6KMOQPEOEKHO","created_at":"2026-05-18T12:29:07Z"},{"alias_kind":"pith_short_16","alias_value":"6KMOQPEOEKHOKSUM","created_at":"2026-05-18T12:29:07Z"},{"alias_kind":"pith_short_8","alias_value":"6KMOQPEO","created_at":"2026-05-18T12:29:07Z"}],"graph_snapshots":[{"event_id":"sha256:f3d71aa17bcdb8fd7d9e9ae2b5e8f5be59670591588cd5b02177a351b2f256bf","target":"graph","created_at":"2026-05-18T01:26:03Z","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 turbulent flow in an infinitely extended plane channel is analysed by solving the Navier-Stokes equations with a DNS approach. Solutions are obtained in a numerical solution domain of finite size in the streamwise as well as in the lateral direction setting periodic boundary conditions in both directions. Their impact on large scale structures in the turbulent flow field is analysed carefully in order to avoid their suppression. When this is done appropriately well known stripe patterns in these flows can be observed and analysed especially with respect to their relative motion compared to","authors_text":"H. Herwig, P. Ki\\v{s}, Y. Jin","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2015-11-24T15:25:59Z","title":"The physics of stripe patterns in turbulent channel flow determined by DNS results"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.07753","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:a6e57564d1cbf1e490530aecb7bb0b4e2e0450ff3b36b7c85f1e9c708780f66d","target":"record","created_at":"2026-05-18T01:26:03Z","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":"6a9b884fdd4d0e56cb104a19f8df3ef837a3ba97e096a9bcc30742140286e5c4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2015-11-24T15:25:59Z","title_canon_sha256":"cefa85d5c3e687c7302052286f813876d49043792ed9364fe74847f7657e3a08"},"schema_version":"1.0","source":{"id":"1511.07753","kind":"arxiv","version":1}},"canonical_sha256":"f298e83c8e228ee54a8c717815ca5e54fe9d4cdcf826d6d857fcff9ca53589a7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f298e83c8e228ee54a8c717815ca5e54fe9d4cdcf826d6d857fcff9ca53589a7","first_computed_at":"2026-05-18T01:26:03.719775Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:26:03.719775Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Un4it6/G4dZIvTpWooSFkjWX3fe1mVb2N9EpSNMFe2OZQa1a1SDbpylg3f3+HDc0VT9oNigyEzRO/f7NqY09AA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:26:03.720279Z","signed_message":"canonical_sha256_bytes"},"source_id":"1511.07753","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a6e57564d1cbf1e490530aecb7bb0b4e2e0450ff3b36b7c85f1e9c708780f66d","sha256:f3d71aa17bcdb8fd7d9e9ae2b5e8f5be59670591588cd5b02177a351b2f256bf"],"state_sha256":"619036680cf1f3b144d0fe1908052fdf6cebd3ba4de38d1c9a18018e43ba6097"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zYwtQRhv/QQzChuJf0cUH+QuuZBfCIOLHgIvqhX7XCICpCz0ngu1yHp/Nt1XzdYlTiZTnLOZi8/QHIYnXHEzAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T21:33:45.970431Z","bundle_sha256":"4637765bbdd6c142faeaaeb6152b6faeeb31ea5974c6c2a9b13c033ca37ff0b3"}}