{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:B7YBAYHBNA4G7S3ZTOLWYM66VX","short_pith_number":"pith:B7YBAYHB","canonical_record":{"source":{"id":"1901.06941","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2019-01-21T14:22:57Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"bdd5febfcf6a32b20aad0164e3fb9a82ae28d8732967042ddaa325bd7b019530","abstract_canon_sha256":"24aad936fa718c2c3dd339856b6809f87dfd6964942d8f07fd86c315a0d51db5"},"schema_version":"1.0"},"canonical_sha256":"0ff01060e168386fcb799b976c33deade741892c1e19ed2e7a3f1af8d84e0502","source":{"kind":"arxiv","id":"1901.06941","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1901.06941","created_at":"2026-05-17T23:55:48Z"},{"alias_kind":"arxiv_version","alias_value":"1901.06941v1","created_at":"2026-05-17T23:55:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.06941","created_at":"2026-05-17T23:55:48Z"},{"alias_kind":"pith_short_12","alias_value":"B7YBAYHBNA4G","created_at":"2026-05-18T12:33:12Z"},{"alias_kind":"pith_short_16","alias_value":"B7YBAYHBNA4G7S3Z","created_at":"2026-05-18T12:33:12Z"},{"alias_kind":"pith_short_8","alias_value":"B7YBAYHB","created_at":"2026-05-18T12:33:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:B7YBAYHBNA4G7S3ZTOLWYM66VX","target":"record","payload":{"canonical_record":{"source":{"id":"1901.06941","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2019-01-21T14:22:57Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"bdd5febfcf6a32b20aad0164e3fb9a82ae28d8732967042ddaa325bd7b019530","abstract_canon_sha256":"24aad936fa718c2c3dd339856b6809f87dfd6964942d8f07fd86c315a0d51db5"},"schema_version":"1.0"},"canonical_sha256":"0ff01060e168386fcb799b976c33deade741892c1e19ed2e7a3f1af8d84e0502","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:55:48.619434Z","signature_b64":"6Ytp03bQil+iC/wwp2CrYYfG1TAbSxTX2ORLGVu6DV9DWo2zp8CfF6BoO4dwLLqjgM9ye7ivpO+6LVzLCqcWCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0ff01060e168386fcb799b976c33deade741892c1e19ed2e7a3f1af8d84e0502","last_reissued_at":"2026-05-17T23:55:48.618658Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:55:48.618658Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1901.06941","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:55:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6w95ZxvhL3y138DJ1qZ/G5pQcPPqjttbBqJNsvr7ijLqWSVZtno3I11r0K/TjTxOzW3pG6ut94j+V9x0niSZBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T20:08:17.404742Z"},"content_sha256":"66042dbaecd5f9118288cd92b097aeaaf2fa97362511d77ae0ca4e19dd3c3f64","schema_version":"1.0","event_id":"sha256:66042dbaecd5f9118288cd92b097aeaaf2fa97362511d77ae0ca4e19dd3c3f64"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:B7YBAYHBNA4G7S3ZTOLWYM66VX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Induced charge electroosmotic flow with finite ion size and solvation effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"physics.chem-ph","authors_text":"Alexander Linke, Christian Merdon, Clemens Guhlke, J\\\"urgen Fuhrmann, R\\\"udiger M\\\"uller","submitted_at":"2019-01-21T14:22:57Z","abstract_excerpt":"The most common mathematical models for electrolyte flows are based on the dilute solution assumption, leading to a coupled system of the Nernst--Planck--Poisson drift-diffusion equations for ion transport and the Stokes resp. Navier--Stokes equations for fluid flow of the solvent. In charged boundary layers the dilute solution assumption is in general not valid and volume exclusion and solvation effects have to be taken into account in a thermodynamically consistent way. Whenever boundary layer effects have a dominant impact on the global behavior of a certain electrochemical system, an accur"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.06941","kind":"arxiv","version":1},"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":"2026-05-17T23:55:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dvxKwlUWBUiaJlBGfA8dbgBLZ+to9iwoLIjmQwrE+XLkvNnrWb/kpbWMdGSTVazYkyJzRfSsluc7D6i+iimwCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T20:08:17.405328Z"},"content_sha256":"96a9328bcbfe6b6f1dc1547bebf26901de67429c93f32be33ca11bfce65c473a","schema_version":"1.0","event_id":"sha256:96a9328bcbfe6b6f1dc1547bebf26901de67429c93f32be33ca11bfce65c473a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX/bundle.json","state_url":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX/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":"2026-05-26T20:08:17Z","links":{"resolver":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX","bundle":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX/bundle.json","state":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:B7YBAYHBNA4G7S3ZTOLWYM66VX","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":"24aad936fa718c2c3dd339856b6809f87dfd6964942d8f07fd86c315a0d51db5","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2019-01-21T14:22:57Z","title_canon_sha256":"bdd5febfcf6a32b20aad0164e3fb9a82ae28d8732967042ddaa325bd7b019530"},"schema_version":"1.0","source":{"id":"1901.06941","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1901.06941","created_at":"2026-05-17T23:55:48Z"},{"alias_kind":"arxiv_version","alias_value":"1901.06941v1","created_at":"2026-05-17T23:55:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.06941","created_at":"2026-05-17T23:55:48Z"},{"alias_kind":"pith_short_12","alias_value":"B7YBAYHBNA4G","created_at":"2026-05-18T12:33:12Z"},{"alias_kind":"pith_short_16","alias_value":"B7YBAYHBNA4G7S3Z","created_at":"2026-05-18T12:33:12Z"},{"alias_kind":"pith_short_8","alias_value":"B7YBAYHB","created_at":"2026-05-18T12:33:12Z"}],"graph_snapshots":[{"event_id":"sha256:96a9328bcbfe6b6f1dc1547bebf26901de67429c93f32be33ca11bfce65c473a","target":"graph","created_at":"2026-05-17T23:55:48Z","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":"The most common mathematical models for electrolyte flows are based on the dilute solution assumption, leading to a coupled system of the Nernst--Planck--Poisson drift-diffusion equations for ion transport and the Stokes resp. Navier--Stokes equations for fluid flow of the solvent. In charged boundary layers the dilute solution assumption is in general not valid and volume exclusion and solvation effects have to be taken into account in a thermodynamically consistent way. Whenever boundary layer effects have a dominant impact on the global behavior of a certain electrochemical system, an accur","authors_text":"Alexander Linke, Christian Merdon, Clemens Guhlke, J\\\"urgen Fuhrmann, R\\\"udiger M\\\"uller","cross_cats":["physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2019-01-21T14:22:57Z","title":"Induced charge electroosmotic flow with finite ion size and solvation effects"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.06941","kind":"arxiv","version":1},"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":"sha256:66042dbaecd5f9118288cd92b097aeaaf2fa97362511d77ae0ca4e19dd3c3f64","target":"record","created_at":"2026-05-17T23:55:48Z","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":"24aad936fa718c2c3dd339856b6809f87dfd6964942d8f07fd86c315a0d51db5","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2019-01-21T14:22:57Z","title_canon_sha256":"bdd5febfcf6a32b20aad0164e3fb9a82ae28d8732967042ddaa325bd7b019530"},"schema_version":"1.0","source":{"id":"1901.06941","kind":"arxiv","version":1}},"canonical_sha256":"0ff01060e168386fcb799b976c33deade741892c1e19ed2e7a3f1af8d84e0502","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0ff01060e168386fcb799b976c33deade741892c1e19ed2e7a3f1af8d84e0502","first_computed_at":"2026-05-17T23:55:48.618658Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:55:48.618658Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6Ytp03bQil+iC/wwp2CrYYfG1TAbSxTX2ORLGVu6DV9DWo2zp8CfF6BoO4dwLLqjgM9ye7ivpO+6LVzLCqcWCw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:55:48.619434Z","signed_message":"canonical_sha256_bytes"},"source_id":"1901.06941","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:66042dbaecd5f9118288cd92b097aeaaf2fa97362511d77ae0ca4e19dd3c3f64","sha256:96a9328bcbfe6b6f1dc1547bebf26901de67429c93f32be33ca11bfce65c473a"],"state_sha256":"91e75a63ba9e104ff9c706f360b682d6fa9d00e7b366ff062a40114adec13852"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sCy1flMtepwQYgMpmzufpckwDDe28eAhFFkvx2f2BOKXuN8LKtgzhl3fUZVFfMj5ZRKqsc4bJK1CwwklHUqkBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T20:08:17.409019Z","bundle_sha256":"54384591bb34b2b0778cbe56df7b8d60aa7a74618b268ffc0e2d2c3f5b3ed9ea"}}