{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:XNKZR35XN3NR3ZHNVY4MPAYWA3","short_pith_number":"pith:XNKZR35X","canonical_record":{"source":{"id":"1109.3277","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2011-09-15T07:29:28Z","cross_cats_sorted":["cs.DC","physics.flu-dyn"],"title_canon_sha256":"e8bb0400ca89dc2d1d0c0edfbf16cf1cfabfb622783e6d19d94d328c7e5630d8","abstract_canon_sha256":"966de1f1e02aa4496cb4891172c2ee75b123d3b0b430404126288b51a6ada852"},"schema_version":"1.0"},"canonical_sha256":"bb5598efb76edb1de4edae38c7831606e0943e8e3302752b692ab5c7d89096d5","source":{"kind":"arxiv","id":"1109.3277","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1109.3277","created_at":"2026-05-18T03:57:00Z"},{"alias_kind":"arxiv_version","alias_value":"1109.3277v2","created_at":"2026-05-18T03:57:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.3277","created_at":"2026-05-18T03:57:00Z"},{"alias_kind":"pith_short_12","alias_value":"XNKZR35XN3NR","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_16","alias_value":"XNKZR35XN3NR3ZHN","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_8","alias_value":"XNKZR35X","created_at":"2026-05-18T12:26:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:XNKZR35XN3NR3ZHNVY4MPAYWA3","target":"record","payload":{"canonical_record":{"source":{"id":"1109.3277","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2011-09-15T07:29:28Z","cross_cats_sorted":["cs.DC","physics.flu-dyn"],"title_canon_sha256":"e8bb0400ca89dc2d1d0c0edfbf16cf1cfabfb622783e6d19d94d328c7e5630d8","abstract_canon_sha256":"966de1f1e02aa4496cb4891172c2ee75b123d3b0b430404126288b51a6ada852"},"schema_version":"1.0"},"canonical_sha256":"bb5598efb76edb1de4edae38c7831606e0943e8e3302752b692ab5c7d89096d5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:57:00.431463Z","signature_b64":"vxtUE5MQy7wKHc+yUgyOBL3oek1UV3KDP/FWiyLT+gD5vg5NG2zZ6TwRdPmw5hrmGw+ZbkRqm6BruuIlF8KJAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bb5598efb76edb1de4edae38c7831606e0943e8e3302752b692ab5c7d89096d5","last_reissued_at":"2026-05-18T03:57:00.430660Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:57:00.430660Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1109.3277","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":"2026-05-18T03:57:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zD71Olou2mNkJpgU+iq/8bmE8DIfk36ZseF7vSr0zKyXMMIT4vNPWKtmXGcq8mCcngE3b1w5PQVBmhM0yNP1DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T18:39:49.993121Z"},"content_sha256":"85eae66536e3beed07ff09d4a5022458928479071832aa4155f939bd46352e04","schema_version":"1.0","event_id":"sha256:85eae66536e3beed07ff09d4a5022458928479071832aa4155f939bd46352e04"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:XNKZR35XN3NR3ZHNVY4MPAYWA3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Lattice Boltzmann simulations of anisotropic particles at liquid interfaces","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cs.DC","physics.flu-dyn"],"primary_cat":"cond-mat.soft","authors_text":"Florian G\\\"unther, Florian Janoschek, Jens Harting, Stefan Frijters","submitted_at":"2011-09-15T07:29:28Z","abstract_excerpt":"Complex colloidal fluids, such as emulsions stabilized by complex shaped particles, play an important role in many industrial applications. However, understanding their physics requires a study at sufficiently large length scales while still resolving the microscopic structure of a large number of particles and of the local hydrodynamics. Due to its high degree of locality, the lattice Boltzmann method, when combined with a molecular dynamics solver and parallelized on modern supercomputers, provides a tool that allows such studies. Still, running simulations on hundreds of thousands of cores "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.3277","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":"2026-05-18T03:57:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qn2+QIWIWX9HD8mWwuKdiT62ixu4P9Qr8R8tgII1qyuxBE/zPwAaq4+Sfaz55OceO+znM3m9RVhkebdeV/IaBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T18:39:49.993854Z"},"content_sha256":"c2ec8e58bfd3699f7488924e5ce289fe443aadeed04aea55cbb5ddf47730e0a1","schema_version":"1.0","event_id":"sha256:c2ec8e58bfd3699f7488924e5ce289fe443aadeed04aea55cbb5ddf47730e0a1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XNKZR35XN3NR3ZHNVY4MPAYWA3/bundle.json","state_url":"https://pith.science/pith/XNKZR35XN3NR3ZHNVY4MPAYWA3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XNKZR35XN3NR3ZHNVY4MPAYWA3/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":"2026-06-09T18:39:49Z","links":{"resolver":"https://pith.science/pith/XNKZR35XN3NR3ZHNVY4MPAYWA3","bundle":"https://pith.science/pith/XNKZR35XN3NR3ZHNVY4MPAYWA3/bundle.json","state":"https://pith.science/pith/XNKZR35XN3NR3ZHNVY4MPAYWA3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XNKZR35XN3NR3ZHNVY4MPAYWA3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:XNKZR35XN3NR3ZHNVY4MPAYWA3","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":"966de1f1e02aa4496cb4891172c2ee75b123d3b0b430404126288b51a6ada852","cross_cats_sorted":["cs.DC","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2011-09-15T07:29:28Z","title_canon_sha256":"e8bb0400ca89dc2d1d0c0edfbf16cf1cfabfb622783e6d19d94d328c7e5630d8"},"schema_version":"1.0","source":{"id":"1109.3277","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1109.3277","created_at":"2026-05-18T03:57:00Z"},{"alias_kind":"arxiv_version","alias_value":"1109.3277v2","created_at":"2026-05-18T03:57:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.3277","created_at":"2026-05-18T03:57:00Z"},{"alias_kind":"pith_short_12","alias_value":"XNKZR35XN3NR","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_16","alias_value":"XNKZR35XN3NR3ZHN","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_8","alias_value":"XNKZR35X","created_at":"2026-05-18T12:26:47Z"}],"graph_snapshots":[{"event_id":"sha256:c2ec8e58bfd3699f7488924e5ce289fe443aadeed04aea55cbb5ddf47730e0a1","target":"graph","created_at":"2026-05-18T03:57:00Z","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":"Complex colloidal fluids, such as emulsions stabilized by complex shaped particles, play an important role in many industrial applications. However, understanding their physics requires a study at sufficiently large length scales while still resolving the microscopic structure of a large number of particles and of the local hydrodynamics. Due to its high degree of locality, the lattice Boltzmann method, when combined with a molecular dynamics solver and parallelized on modern supercomputers, provides a tool that allows such studies. Still, running simulations on hundreds of thousands of cores ","authors_text":"Florian G\\\"unther, Florian Janoschek, Jens Harting, Stefan Frijters","cross_cats":["cs.DC","physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2011-09-15T07:29:28Z","title":"Lattice Boltzmann simulations of anisotropic particles at liquid interfaces"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.3277","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":"sha256:85eae66536e3beed07ff09d4a5022458928479071832aa4155f939bd46352e04","target":"record","created_at":"2026-05-18T03:57:00Z","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":"966de1f1e02aa4496cb4891172c2ee75b123d3b0b430404126288b51a6ada852","cross_cats_sorted":["cs.DC","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2011-09-15T07:29:28Z","title_canon_sha256":"e8bb0400ca89dc2d1d0c0edfbf16cf1cfabfb622783e6d19d94d328c7e5630d8"},"schema_version":"1.0","source":{"id":"1109.3277","kind":"arxiv","version":2}},"canonical_sha256":"bb5598efb76edb1de4edae38c7831606e0943e8e3302752b692ab5c7d89096d5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bb5598efb76edb1de4edae38c7831606e0943e8e3302752b692ab5c7d89096d5","first_computed_at":"2026-05-18T03:57:00.430660Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:57:00.430660Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vxtUE5MQy7wKHc+yUgyOBL3oek1UV3KDP/FWiyLT+gD5vg5NG2zZ6TwRdPmw5hrmGw+ZbkRqm6BruuIlF8KJAA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:57:00.431463Z","signed_message":"canonical_sha256_bytes"},"source_id":"1109.3277","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:85eae66536e3beed07ff09d4a5022458928479071832aa4155f939bd46352e04","sha256:c2ec8e58bfd3699f7488924e5ce289fe443aadeed04aea55cbb5ddf47730e0a1"],"state_sha256":"7d89f8658628550a5f864b41cf611cdd72fbafedc22e8f68f4e87d32c2fd2dc9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PVH61YZvryUY1tO+cT3ju+YkAy6Ex9s/SQc/2GjUAc1gCE+Xi85qXlXuRUH7zBg6L/eE6DiqZp/rW/cDTa1ECA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T18:39:49.997979Z","bundle_sha256":"2b6593eedc53e0b4292fb2f92a36e785c3c4e3eba34400b120e2ae90b32da7c0"}}