{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:CSZ6CJQHOGTKO5W5JXW6F3YLAV","short_pith_number":"pith:CSZ6CJQH","canonical_record":{"source":{"id":"1312.0199","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2013-12-01T10:48:25Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"80cbdcbc0815be1bc1d24dab1bc9788ae0e5111ffb8d56817a54bdb09b621876","abstract_canon_sha256":"578a483bbde1ae5f23b8a89cd61eabcf484732a17cd93a18f1b3db029c198483"},"schema_version":"1.0"},"canonical_sha256":"14b3e1260771a6a776dd4dede2ef0b0560123b39d3e64672c118932f52cad9d9","source":{"kind":"arxiv","id":"1312.0199","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.0199","created_at":"2026-05-18T03:01:23Z"},{"alias_kind":"arxiv_version","alias_value":"1312.0199v2","created_at":"2026-05-18T03:01:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.0199","created_at":"2026-05-18T03:01:23Z"},{"alias_kind":"pith_short_12","alias_value":"CSZ6CJQHOGTK","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_16","alias_value":"CSZ6CJQHOGTKO5W5","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_8","alias_value":"CSZ6CJQH","created_at":"2026-05-18T12:27:40Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:CSZ6CJQHOGTKO5W5JXW6F3YLAV","target":"record","payload":{"canonical_record":{"source":{"id":"1312.0199","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2013-12-01T10:48:25Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"80cbdcbc0815be1bc1d24dab1bc9788ae0e5111ffb8d56817a54bdb09b621876","abstract_canon_sha256":"578a483bbde1ae5f23b8a89cd61eabcf484732a17cd93a18f1b3db029c198483"},"schema_version":"1.0"},"canonical_sha256":"14b3e1260771a6a776dd4dede2ef0b0560123b39d3e64672c118932f52cad9d9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:01:23.944805Z","signature_b64":"MouFmt+Yh+W61dqiCDcxtsBk8jQmo6qNthRBvvVBom+GocPcLTal7UeFMXgaZRk28Rf2BgeVThM8f4MM76TiCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"14b3e1260771a6a776dd4dede2ef0b0560123b39d3e64672c118932f52cad9d9","last_reissued_at":"2026-05-18T03:01:23.944119Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:01:23.944119Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1312.0199","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:01:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Rso3wUewQKBh5NdRnQMk4fDmGcGIAliRMMptOMmLzpC5v99D4J8Ns1gVCgGdn9d3bm3dXNfiYWSq5wkuecwyCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T10:40:15.049929Z"},"content_sha256":"3c3b917bd09e8bc4f6ff894e812b77153649c79eb099ce2445608d16928fe648","schema_version":"1.0","event_id":"sha256:3c3b917bd09e8bc4f6ff894e812b77153649c79eb099ce2445608d16928fe648"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:CSZ6CJQHOGTKO5W5JXW6F3YLAV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Lattice-Boltzmann simulations of the drag force on a sphere approaching a superhydrophobic striped plane","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft"],"primary_cat":"physics.flu-dyn","authors_text":"Alexander L. Dubov, Evgeny S. Asmolov, Jens Harting, Olga I. Vinogradova, Sebastian Schmieschek","submitted_at":"2013-12-01T10:48:25Z","abstract_excerpt":"By means of lattice-Boltzmann simulations the drag force on a sphere of radius R approaching a superhydrophobic striped wall has been investigated as a function of arbitrary separation h. Superhydrophobic (perfect-slip vs. no-slip) stripes are characterized by a texture period L and a fraction of the gas area $\\phi$. For very large values of h/R we recover the macroscopic formulae for a sphere moving towards a hydrophilic no-slip plane. For h/R=O(1) and smaller the drag force is smaller than predicted by classical theories for hydrophilic no-slip surfaces, but larger than expected for a sphere"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.0199","kind":"arxiv","version":2},"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":"2026-05-18T03:01:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"V+S+6ov1zEOdqadQptTEEsy1IKM+UXikdMTX385wb8TDgcGYWN5zY5jxEQCSFxNgBDLmF5sqh5cPJzYJkEP5Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T10:40:15.050568Z"},"content_sha256":"5e4dfb840770a108bf6003a7af7b1375bd80bb9d1c0de143e9da84f43a1aecb1","schema_version":"1.0","event_id":"sha256:5e4dfb840770a108bf6003a7af7b1375bd80bb9d1c0de143e9da84f43a1aecb1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CSZ6CJQHOGTKO5W5JXW6F3YLAV/bundle.json","state_url":"https://pith.science/pith/CSZ6CJQHOGTKO5W5JXW6F3YLAV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CSZ6CJQHOGTKO5W5JXW6F3YLAV/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":"2026-05-22T10:40:15Z","links":{"resolver":"https://pith.science/pith/CSZ6CJQHOGTKO5W5JXW6F3YLAV","bundle":"https://pith.science/pith/CSZ6CJQHOGTKO5W5JXW6F3YLAV/bundle.json","state":"https://pith.science/pith/CSZ6CJQHOGTKO5W5JXW6F3YLAV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CSZ6CJQHOGTKO5W5JXW6F3YLAV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:CSZ6CJQHOGTKO5W5JXW6F3YLAV","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":"578a483bbde1ae5f23b8a89cd61eabcf484732a17cd93a18f1b3db029c198483","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2013-12-01T10:48:25Z","title_canon_sha256":"80cbdcbc0815be1bc1d24dab1bc9788ae0e5111ffb8d56817a54bdb09b621876"},"schema_version":"1.0","source":{"id":"1312.0199","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.0199","created_at":"2026-05-18T03:01:23Z"},{"alias_kind":"arxiv_version","alias_value":"1312.0199v2","created_at":"2026-05-18T03:01:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.0199","created_at":"2026-05-18T03:01:23Z"},{"alias_kind":"pith_short_12","alias_value":"CSZ6CJQHOGTK","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_16","alias_value":"CSZ6CJQHOGTKO5W5","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_8","alias_value":"CSZ6CJQH","created_at":"2026-05-18T12:27:40Z"}],"graph_snapshots":[{"event_id":"sha256:5e4dfb840770a108bf6003a7af7b1375bd80bb9d1c0de143e9da84f43a1aecb1","target":"graph","created_at":"2026-05-18T03:01:23Z","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":"By means of lattice-Boltzmann simulations the drag force on a sphere of radius R approaching a superhydrophobic striped wall has been investigated as a function of arbitrary separation h. Superhydrophobic (perfect-slip vs. no-slip) stripes are characterized by a texture period L and a fraction of the gas area $\\phi$. For very large values of h/R we recover the macroscopic formulae for a sphere moving towards a hydrophilic no-slip plane. For h/R=O(1) and smaller the drag force is smaller than predicted by classical theories for hydrophilic no-slip surfaces, but larger than expected for a sphere","authors_text":"Alexander L. Dubov, Evgeny S. Asmolov, Jens Harting, Olga I. Vinogradova, Sebastian Schmieschek","cross_cats":["cond-mat.soft"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2013-12-01T10:48:25Z","title":"Lattice-Boltzmann simulations of the drag force on a sphere approaching a superhydrophobic striped plane"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.0199","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":"sha256:3c3b917bd09e8bc4f6ff894e812b77153649c79eb099ce2445608d16928fe648","target":"record","created_at":"2026-05-18T03:01:23Z","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":"578a483bbde1ae5f23b8a89cd61eabcf484732a17cd93a18f1b3db029c198483","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2013-12-01T10:48:25Z","title_canon_sha256":"80cbdcbc0815be1bc1d24dab1bc9788ae0e5111ffb8d56817a54bdb09b621876"},"schema_version":"1.0","source":{"id":"1312.0199","kind":"arxiv","version":2}},"canonical_sha256":"14b3e1260771a6a776dd4dede2ef0b0560123b39d3e64672c118932f52cad9d9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"14b3e1260771a6a776dd4dede2ef0b0560123b39d3e64672c118932f52cad9d9","first_computed_at":"2026-05-18T03:01:23.944119Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:01:23.944119Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MouFmt+Yh+W61dqiCDcxtsBk8jQmo6qNthRBvvVBom+GocPcLTal7UeFMXgaZRk28Rf2BgeVThM8f4MM76TiCg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:01:23.944805Z","signed_message":"canonical_sha256_bytes"},"source_id":"1312.0199","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3c3b917bd09e8bc4f6ff894e812b77153649c79eb099ce2445608d16928fe648","sha256:5e4dfb840770a108bf6003a7af7b1375bd80bb9d1c0de143e9da84f43a1aecb1"],"state_sha256":"017b945ed74810dffff58869b0794aa8e8904ab11f09254d8602823df3ebab4b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rWP0T/SFr9BcgJYxgawyAvLN21RG/8KSaViykiKu4KoQrTnkIG8Y5SPIFROMvZW3PHogspRFi1ryYaTW1H89CA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-22T10:40:15.053812Z","bundle_sha256":"f55312115355a3ca1ea8d4ad572d381031dccb4232f981348eae62e61d7e150c"}}