{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:Y5PA362ZBWSFOQ5A6D4BP752AA","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":"15b0366b47fe82b5eb660f1e3c3c7fb06c873b9fd26b7ec6beea24ef4ba4b52b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2018-06-30T16:52:47Z","title_canon_sha256":"872502f62f924916fa26cf623609b90f268ba57f690a1283f500a667cec18b82"},"schema_version":"1.0","source":{"id":"1807.00203","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.00203","created_at":"2026-05-17T23:53:12Z"},{"alias_kind":"arxiv_version","alias_value":"1807.00203v2","created_at":"2026-05-17T23:53:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.00203","created_at":"2026-05-17T23:53:12Z"},{"alias_kind":"pith_short_12","alias_value":"Y5PA362ZBWSF","created_at":"2026-05-18T12:33:04Z"},{"alias_kind":"pith_short_16","alias_value":"Y5PA362ZBWSFOQ5A","created_at":"2026-05-18T12:33:04Z"},{"alias_kind":"pith_short_8","alias_value":"Y5PA362Z","created_at":"2026-05-18T12:33:04Z"}],"graph_snapshots":[{"event_id":"sha256:1fe5ccad9e86d4793dcbc431c6bcf1948d16113016a8c24f13283d2c630efc89","target":"graph","created_at":"2026-05-17T23:53:12Z","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 discuss two distinct spatial structures of vortex streets. The `conventional mushroom' structure is commonly discuss in many experimental studies, but the exotic `separated rows' structure is characterized by a thin irrotational fluid between two rows of vortices. In a two-dimensional soap film channel, we generated the exotic vortex arrangement by using triangular objects. This setup allows us to vary the thickness of boundary layers and their separation distance independently. We find that the separated rows structure appears only when the boundary layer thickness is less than 40% of the ","authors_text":"Ildoo Kim","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2018-06-30T16:52:47Z","title":"Separated Rows structure of vortex streets behind triangular objects"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.00203","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":"sha256:6d585245bc1b87bc2d6d3901e8cdd1daab01bad2bf4d79502e1fde5941f1afd9","target":"record","created_at":"2026-05-17T23:53:12Z","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":"15b0366b47fe82b5eb660f1e3c3c7fb06c873b9fd26b7ec6beea24ef4ba4b52b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2018-06-30T16:52:47Z","title_canon_sha256":"872502f62f924916fa26cf623609b90f268ba57f690a1283f500a667cec18b82"},"schema_version":"1.0","source":{"id":"1807.00203","kind":"arxiv","version":2}},"canonical_sha256":"c75e0dfb590da45743a0f0f817ffba001acebaed7f0b59203c7cd6ced62989f8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c75e0dfb590da45743a0f0f817ffba001acebaed7f0b59203c7cd6ced62989f8","first_computed_at":"2026-05-17T23:53:12.463348Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:53:12.463348Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"42ZgYN7Cw08gHWH5MaP8M+7VWxkgeI1PNm1LsCXNg20Y1O1n3EiTRZBjJ+iORFciz63e1fmYeKiFjhVgVOE7CQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:53:12.463994Z","signed_message":"canonical_sha256_bytes"},"source_id":"1807.00203","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6d585245bc1b87bc2d6d3901e8cdd1daab01bad2bf4d79502e1fde5941f1afd9","sha256:1fe5ccad9e86d4793dcbc431c6bcf1948d16113016a8c24f13283d2c630efc89"],"state_sha256":"12b729a8ff597ac54ff07c1ea7e0d4c44f1106338c36709daa5e816853ef9a9c"}