{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:E2SEW2ELWBEPVXMRY45BA2JQJM","short_pith_number":"pith:E2SEW2EL","canonical_record":{"source":{"id":"1211.5224","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-11-22T08:15:55Z","cross_cats_sorted":["physics.flu-dyn"],"title_canon_sha256":"d6479011785451a9b0b480ceb5d80d91878a7a4755980518cb5873ff08b1ce7d","abstract_canon_sha256":"cf44c55b40e7e4207c434cfc3f5c959ff3f099d8fccb6c6685c29e81c8c5fe36"},"schema_version":"1.0"},"canonical_sha256":"26a44b688bb048fadd91c73a1069304b0ce2f7afa6adfc56aeb469419bc6b86c","source":{"kind":"arxiv","id":"1211.5224","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.5224","created_at":"2026-05-18T03:37:40Z"},{"alias_kind":"arxiv_version","alias_value":"1211.5224v1","created_at":"2026-05-18T03:37:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.5224","created_at":"2026-05-18T03:37:40Z"},{"alias_kind":"pith_short_12","alias_value":"E2SEW2ELWBEP","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_16","alias_value":"E2SEW2ELWBEPVXMR","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_8","alias_value":"E2SEW2EL","created_at":"2026-05-18T12:27:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:E2SEW2ELWBEPVXMRY45BA2JQJM","target":"record","payload":{"canonical_record":{"source":{"id":"1211.5224","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-11-22T08:15:55Z","cross_cats_sorted":["physics.flu-dyn"],"title_canon_sha256":"d6479011785451a9b0b480ceb5d80d91878a7a4755980518cb5873ff08b1ce7d","abstract_canon_sha256":"cf44c55b40e7e4207c434cfc3f5c959ff3f099d8fccb6c6685c29e81c8c5fe36"},"schema_version":"1.0"},"canonical_sha256":"26a44b688bb048fadd91c73a1069304b0ce2f7afa6adfc56aeb469419bc6b86c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:37:40.613027Z","signature_b64":"mBKythdQORnmPk+oF3RPJUTamEhfQNe5la4zN1JcGAiYcGgy5frSYZF1QsYkwXu12zErxAykcRguGEMPzrTJCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"26a44b688bb048fadd91c73a1069304b0ce2f7afa6adfc56aeb469419bc6b86c","last_reissued_at":"2026-05-18T03:37:40.612567Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:37:40.612567Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1211.5224","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":"2026-05-18T03:37:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MPMawlwfZBfUjUR/0R1eSp9ohWi6/2HoaCUylUN7gOP3e9eWitoUFx9z64WWFVqBhG/CFpblxsr218VW0lWEBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T08:45:44.000827Z"},"content_sha256":"7e5c7c20e75b49d50d5497efc105988a12679571263986ceb4b4f2298d7d2ee7","schema_version":"1.0","event_id":"sha256:7e5c7c20e75b49d50d5497efc105988a12679571263986ceb4b4f2298d7d2ee7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:E2SEW2ELWBEPVXMRY45BA2JQJM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Taylor Dispersion with Adsorption and Desorption","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.flu-dyn"],"primary_cat":"cond-mat.stat-mech","authors_text":"Benjamin Rotenberg, Maximilien Levesque, Olivier B\\'enichou, Rapha\\\"el Voituriez","submitted_at":"2012-11-22T08:15:55Z","abstract_excerpt":"We use a stochastic approach to show how Taylor dispersion is affected by kinetic processes of adsorption and desorption onto surfaces. A general theory is developed, from which we derive explicitly the dispersion coefficients of canonical examples like Poiseuille flows in planar and cylindrical geometries, both in constant and sinusoidal velocity fields. These results open the way for the measurement of adsorption and desorption rate constants using stationary flows and molecular sorting using the stochastic resonance of the adsorption and desorption processes with the oscillatory velocity fi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.5224","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":"2026-05-18T03:37:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FqvCsMHkDn1mIeiNQieiP4j7fhSK+PH3bJqtmc46Gh/eOU3fS28mfwDH1xrld5Qg3MWggptmFpyDxKA/JNPFBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T08:45:44.001175Z"},"content_sha256":"52e22be2b15a6f43098e92197b5f731029e8881e57ed33e836efd0e7e43d06e2","schema_version":"1.0","event_id":"sha256:52e22be2b15a6f43098e92197b5f731029e8881e57ed33e836efd0e7e43d06e2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/E2SEW2ELWBEPVXMRY45BA2JQJM/bundle.json","state_url":"https://pith.science/pith/E2SEW2ELWBEPVXMRY45BA2JQJM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/E2SEW2ELWBEPVXMRY45BA2JQJM/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":"2026-05-30T08:45:44Z","links":{"resolver":"https://pith.science/pith/E2SEW2ELWBEPVXMRY45BA2JQJM","bundle":"https://pith.science/pith/E2SEW2ELWBEPVXMRY45BA2JQJM/bundle.json","state":"https://pith.science/pith/E2SEW2ELWBEPVXMRY45BA2JQJM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/E2SEW2ELWBEPVXMRY45BA2JQJM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:E2SEW2ELWBEPVXMRY45BA2JQJM","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":"cf44c55b40e7e4207c434cfc3f5c959ff3f099d8fccb6c6685c29e81c8c5fe36","cross_cats_sorted":["physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-11-22T08:15:55Z","title_canon_sha256":"d6479011785451a9b0b480ceb5d80d91878a7a4755980518cb5873ff08b1ce7d"},"schema_version":"1.0","source":{"id":"1211.5224","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.5224","created_at":"2026-05-18T03:37:40Z"},{"alias_kind":"arxiv_version","alias_value":"1211.5224v1","created_at":"2026-05-18T03:37:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.5224","created_at":"2026-05-18T03:37:40Z"},{"alias_kind":"pith_short_12","alias_value":"E2SEW2ELWBEP","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_16","alias_value":"E2SEW2ELWBEPVXMR","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_8","alias_value":"E2SEW2EL","created_at":"2026-05-18T12:27:04Z"}],"graph_snapshots":[{"event_id":"sha256:52e22be2b15a6f43098e92197b5f731029e8881e57ed33e836efd0e7e43d06e2","target":"graph","created_at":"2026-05-18T03:37:40Z","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":"We use a stochastic approach to show how Taylor dispersion is affected by kinetic processes of adsorption and desorption onto surfaces. A general theory is developed, from which we derive explicitly the dispersion coefficients of canonical examples like Poiseuille flows in planar and cylindrical geometries, both in constant and sinusoidal velocity fields. These results open the way for the measurement of adsorption and desorption rate constants using stationary flows and molecular sorting using the stochastic resonance of the adsorption and desorption processes with the oscillatory velocity fi","authors_text":"Benjamin Rotenberg, Maximilien Levesque, Olivier B\\'enichou, Rapha\\\"el Voituriez","cross_cats":["physics.flu-dyn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-11-22T08:15:55Z","title":"Taylor Dispersion with Adsorption and Desorption"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.5224","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":"sha256:7e5c7c20e75b49d50d5497efc105988a12679571263986ceb4b4f2298d7d2ee7","target":"record","created_at":"2026-05-18T03:37:40Z","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":"cf44c55b40e7e4207c434cfc3f5c959ff3f099d8fccb6c6685c29e81c8c5fe36","cross_cats_sorted":["physics.flu-dyn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-11-22T08:15:55Z","title_canon_sha256":"d6479011785451a9b0b480ceb5d80d91878a7a4755980518cb5873ff08b1ce7d"},"schema_version":"1.0","source":{"id":"1211.5224","kind":"arxiv","version":1}},"canonical_sha256":"26a44b688bb048fadd91c73a1069304b0ce2f7afa6adfc56aeb469419bc6b86c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"26a44b688bb048fadd91c73a1069304b0ce2f7afa6adfc56aeb469419bc6b86c","first_computed_at":"2026-05-18T03:37:40.612567Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:37:40.612567Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mBKythdQORnmPk+oF3RPJUTamEhfQNe5la4zN1JcGAiYcGgy5frSYZF1QsYkwXu12zErxAykcRguGEMPzrTJCw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:37:40.613027Z","signed_message":"canonical_sha256_bytes"},"source_id":"1211.5224","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7e5c7c20e75b49d50d5497efc105988a12679571263986ceb4b4f2298d7d2ee7","sha256:52e22be2b15a6f43098e92197b5f731029e8881e57ed33e836efd0e7e43d06e2"],"state_sha256":"6c7c3c1e53ef83ff3ab9a308de0189b77f946a0e3928fd77ce537dfc3346f900"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cW6Zdotx6THOatwvbrd5wPL4gVG2ay7P5Fss19As03hbp8qb+cykSLvRJtTjrikka3pD4daxHgOrMH2d1CPiAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T08:45:44.003191Z","bundle_sha256":"d7ef1ed3b9de8a46a6eaa33abdfcfcac9c9890cfd2285acbb9ca14677136a92d"}}