{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:PI6UWY4D2LAUHJYGC2NBJY2EHV","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":"3444998850b1eaa872d7147f90a4cc76c70730544605ab01788026a5ea716f11","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci","cond-mat.soft","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2014-04-16T02:11:49Z","title_canon_sha256":"16b99a7cc0ec62d75fbb924580b05b619354f7c92032705f14ac0ca725c5aa13"},"schema_version":"1.0","source":{"id":"1404.4124","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.4124","created_at":"2026-05-18T02:50:30Z"},{"alias_kind":"arxiv_version","alias_value":"1404.4124v3","created_at":"2026-05-18T02:50:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.4124","created_at":"2026-05-18T02:50:30Z"},{"alias_kind":"pith_short_12","alias_value":"PI6UWY4D2LAU","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"PI6UWY4D2LAUHJYG","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"PI6UWY4D","created_at":"2026-05-18T12:28:43Z"}],"graph_snapshots":[{"event_id":"sha256:fd06d5262c719371dcb2128cb11eb77f08fef5efee41c6e2c0abf839f09ec62d","target":"graph","created_at":"2026-05-18T02:50:30Z","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":"Electrokinetic flows of an aqueous NaCl solution in nanochannels with negatively charged surfaces are studied using molecular dynamics (MD) simulations. The four transport coefficients that characterise the response to weak electric and pressure fields, namely the coefficients for the electrical current in response to the electric field ($M^{jj}$) and the pressure field ($M^{jm}$), and those for the mass flow in response to the same fields ($M^{mj}$ and $M^{mm}$), are obtained in the linear regime using a Green--Kubo approach. Nonequilibrium simulations with explicit external fields are also c","authors_text":"Hideyuki Mizuno, Hiroaki Yoshida, Hitoshi Washizu, Jean-Louis Barrat, Tomoyuki Kinjo","cross_cats":["cond-mat.mes-hall","cond-mat.mtrl-sci","cond-mat.soft","physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2014-04-16T02:11:49Z","title":"Molecular dynamics simulation of electrokinetic flow of an aqueous electrolyte solution in nanochannels"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.4124","kind":"arxiv","version":3},"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:a82f757a11943c6bda004169a51a0afef1302d095a1b4b2abe48e6f7905f75fe","target":"record","created_at":"2026-05-18T02:50:30Z","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":"3444998850b1eaa872d7147f90a4cc76c70730544605ab01788026a5ea716f11","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci","cond-mat.soft","physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2014-04-16T02:11:49Z","title_canon_sha256":"16b99a7cc0ec62d75fbb924580b05b619354f7c92032705f14ac0ca725c5aa13"},"schema_version":"1.0","source":{"id":"1404.4124","kind":"arxiv","version":3}},"canonical_sha256":"7a3d4b6383d2c143a706169a14e3443d7e9fc2df29776f8874cb70fd803e50b5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7a3d4b6383d2c143a706169a14e3443d7e9fc2df29776f8874cb70fd803e50b5","first_computed_at":"2026-05-18T02:50:30.993960Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:50:30.993960Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Jim3TsnNEYEhtELkbFrYyxMKLT5X95tHHg7f4DDeW7a3iZiSQCTjQAh844pQf7XPWarMpiqXe6U0AsM1CDnzBg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:50:30.994596Z","signed_message":"canonical_sha256_bytes"},"source_id":"1404.4124","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a82f757a11943c6bda004169a51a0afef1302d095a1b4b2abe48e6f7905f75fe","sha256:fd06d5262c719371dcb2128cb11eb77f08fef5efee41c6e2c0abf839f09ec62d"],"state_sha256":"bdae67650d32befac1a83e735fcf26403625ce785ad04fc0409eaa50ea8c97f5"}