{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:HVEDPQRUJ2AN5BF6FZHVXJHMQY","short_pith_number":"pith:HVEDPQRU","canonical_record":{"source":{"id":"1506.03661","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-06-11T13:12:58Z","cross_cats_sorted":["cond-mat.mes-hall","physics.flu-dyn"],"title_canon_sha256":"7fb11aa53d23f97e27ae27e88ac1a3e7f8ac62b9be8d2dc32ea7a8c6f808fee9","abstract_canon_sha256":"0049e5f12a256e98136c331c82679b477c78217c26078f1ac4ebce9c42930ab1"},"schema_version":"1.0"},"canonical_sha256":"3d4837c2344e80de84be2e4f5ba4ec86162a07f8689cf8cf575a39ad515bbfe9","source":{"kind":"arxiv","id":"1506.03661","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1506.03661","created_at":"2026-05-18T00:53:35Z"},{"alias_kind":"arxiv_version","alias_value":"1506.03661v2","created_at":"2026-05-18T00:53:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.03661","created_at":"2026-05-18T00:53:35Z"},{"alias_kind":"pith_short_12","alias_value":"HVEDPQRUJ2AN","created_at":"2026-05-18T12:29:25Z"},{"alias_kind":"pith_short_16","alias_value":"HVEDPQRUJ2AN5BF6","created_at":"2026-05-18T12:29:25Z"},{"alias_kind":"pith_short_8","alias_value":"HVEDPQRU","created_at":"2026-05-18T12:29:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:HVEDPQRUJ2AN5BF6FZHVXJHMQY","target":"record","payload":{"canonical_record":{"source":{"id":"1506.03661","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-06-11T13:12:58Z","cross_cats_sorted":["cond-mat.mes-hall","physics.flu-dyn"],"title_canon_sha256":"7fb11aa53d23f97e27ae27e88ac1a3e7f8ac62b9be8d2dc32ea7a8c6f808fee9","abstract_canon_sha256":"0049e5f12a256e98136c331c82679b477c78217c26078f1ac4ebce9c42930ab1"},"schema_version":"1.0"},"canonical_sha256":"3d4837c2344e80de84be2e4f5ba4ec86162a07f8689cf8cf575a39ad515bbfe9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:53:35.044998Z","signature_b64":"RtPXRhk3lPGUhRjjcNO9Xyxr9MQMe8mX+JN6JbdK4R0T5uWiLxjAnznEX9M2Q/GGRVbOnnNmZKFUQGBm11SDDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3d4837c2344e80de84be2e4f5ba4ec86162a07f8689cf8cf575a39ad515bbfe9","last_reissued_at":"2026-05-18T00:53:35.044608Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:53:35.044608Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1506.03661","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":"2026-05-18T00:53:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wyAsGFPkpz31/E1L2qqMGfiE2IouGKNrpgUir+HRmkVi4LjriJXMdqUtYa0zLBonQk1c8EuN5fukXohqIr6UBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T11:06:22.302113Z"},"content_sha256":"00c7a416ef84cc84a5c5f22a423ad1adc7a60673bdfea2b7aee1bab811c1bbf4","schema_version":"1.0","event_id":"sha256:00c7a416ef84cc84a5c5f22a423ad1adc7a60673bdfea2b7aee1bab811c1bbf4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:HVEDPQRUJ2AN5BF6FZHVXJHMQY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Continuum Nanofluidics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","physics.flu-dyn"],"primary_cat":"cond-mat.soft","authors_text":"B. D. Todd, Henrik Bruus, Jeppe C. Dyre, J.S. Hansen, Peter J. Daivis","submitted_at":"2015-06-11T13:12:58Z","abstract_excerpt":"This paper introduces the fundamental continuum theory governing momentum transport in isotropic nanofluidic flows. The theory is an extension to the classical Navier-Stokes equation, which includes coupling between translational and rotational degrees of freedom, as well as non-local response functions that incorporates spatial correlations. The continuum theory is compared with molecular dynamics simulation data for both relaxation processes and fluid flows showing excellent agreement on the nanometer length scale. We also present practical tools to estimate when the extended theory should b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.03661","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":"2026-05-18T00:53:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"H2Gb151UHzLZNfA1CSP3csMBvCTE/n4XBSPkbfnOfYYyz3cwOM/BQt/l5wJ1XlE+kaQJ/nyQL23JwggxkWF5BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T11:06:22.302894Z"},"content_sha256":"be70f7a0d222eb7ea78a067dd155c060888b2537fa6594d2097f2910ecba16a6","schema_version":"1.0","event_id":"sha256:be70f7a0d222eb7ea78a067dd155c060888b2537fa6594d2097f2910ecba16a6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HVEDPQRUJ2AN5BF6FZHVXJHMQY/bundle.json","state_url":"https://pith.science/pith/HVEDPQRUJ2AN5BF6FZHVXJHMQY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HVEDPQRUJ2AN5BF6FZHVXJHMQY/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":"2026-06-10T11:06:22Z","links":{"resolver":"https://pith.science/pith/HVEDPQRUJ2AN5BF6FZHVXJHMQY","bundle":"https://pith.science/pith/HVEDPQRUJ2AN5BF6FZHVXJHMQY/bundle.json","state":"https://pith.science/pith/HVEDPQRUJ2AN5BF6FZHVXJHMQY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HVEDPQRUJ2AN5BF6FZHVXJHMQY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:HVEDPQRUJ2AN5BF6FZHVXJHMQY","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":"0049e5f12a256e98136c331c82679b477c78217c26078f1ac4ebce9c42930ab1","cross_cats_sorted":["cond-mat.mes-hall","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-06-11T13:12:58Z","title_canon_sha256":"7fb11aa53d23f97e27ae27e88ac1a3e7f8ac62b9be8d2dc32ea7a8c6f808fee9"},"schema_version":"1.0","source":{"id":"1506.03661","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1506.03661","created_at":"2026-05-18T00:53:35Z"},{"alias_kind":"arxiv_version","alias_value":"1506.03661v2","created_at":"2026-05-18T00:53:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.03661","created_at":"2026-05-18T00:53:35Z"},{"alias_kind":"pith_short_12","alias_value":"HVEDPQRUJ2AN","created_at":"2026-05-18T12:29:25Z"},{"alias_kind":"pith_short_16","alias_value":"HVEDPQRUJ2AN5BF6","created_at":"2026-05-18T12:29:25Z"},{"alias_kind":"pith_short_8","alias_value":"HVEDPQRU","created_at":"2026-05-18T12:29:25Z"}],"graph_snapshots":[{"event_id":"sha256:be70f7a0d222eb7ea78a067dd155c060888b2537fa6594d2097f2910ecba16a6","target":"graph","created_at":"2026-05-18T00:53:35Z","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":"This paper introduces the fundamental continuum theory governing momentum transport in isotropic nanofluidic flows. The theory is an extension to the classical Navier-Stokes equation, which includes coupling between translational and rotational degrees of freedom, as well as non-local response functions that incorporates spatial correlations. The continuum theory is compared with molecular dynamics simulation data for both relaxation processes and fluid flows showing excellent agreement on the nanometer length scale. We also present practical tools to estimate when the extended theory should b","authors_text":"B. D. Todd, Henrik Bruus, Jeppe C. Dyre, J.S. Hansen, Peter J. Daivis","cross_cats":["cond-mat.mes-hall","physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-06-11T13:12:58Z","title":"Continuum Nanofluidics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.03661","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":"sha256:00c7a416ef84cc84a5c5f22a423ad1adc7a60673bdfea2b7aee1bab811c1bbf4","target":"record","created_at":"2026-05-18T00:53:35Z","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":"0049e5f12a256e98136c331c82679b477c78217c26078f1ac4ebce9c42930ab1","cross_cats_sorted":["cond-mat.mes-hall","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-06-11T13:12:58Z","title_canon_sha256":"7fb11aa53d23f97e27ae27e88ac1a3e7f8ac62b9be8d2dc32ea7a8c6f808fee9"},"schema_version":"1.0","source":{"id":"1506.03661","kind":"arxiv","version":2}},"canonical_sha256":"3d4837c2344e80de84be2e4f5ba4ec86162a07f8689cf8cf575a39ad515bbfe9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3d4837c2344e80de84be2e4f5ba4ec86162a07f8689cf8cf575a39ad515bbfe9","first_computed_at":"2026-05-18T00:53:35.044608Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:53:35.044608Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"RtPXRhk3lPGUhRjjcNO9Xyxr9MQMe8mX+JN6JbdK4R0T5uWiLxjAnznEX9M2Q/GGRVbOnnNmZKFUQGBm11SDDw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:53:35.044998Z","signed_message":"canonical_sha256_bytes"},"source_id":"1506.03661","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:00c7a416ef84cc84a5c5f22a423ad1adc7a60673bdfea2b7aee1bab811c1bbf4","sha256:be70f7a0d222eb7ea78a067dd155c060888b2537fa6594d2097f2910ecba16a6"],"state_sha256":"3b7b58bde6889cbc2481abf4a289e1b2b198cbf9d7233d38e46e772823d7857b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WriNIRtTo/MJze2yApsfjfYVOHuuWFCZ0lunT+L4/GAtaBQg+QRK1+2XGw9BWJLzjZTuDbxhZioZqidCOhghBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T11:06:22.307225Z","bundle_sha256":"a9279ed12edf9c412f3d9f65f870948f3fe2e0b673f0db9bc4714105eb542e79"}}