{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:6OZA4HANAT3OKN4RBEXJ2SNROT","short_pith_number":"pith:6OZA4HAN","canonical_record":{"source":{"id":"1405.1372","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2014-05-06T17:27:11Z","cross_cats_sorted":[],"title_canon_sha256":"54ff0caf6204ef76d32550faae09e8710ee3225ba5c24f17b68302190282ec09","abstract_canon_sha256":"3e9ebb22a61a0cc762e017d9e1f28cf2254748c0a6232be9da44bae539007d4e"},"schema_version":"1.0"},"canonical_sha256":"f3b20e1c0d04f6e53791092e9d49b174d48eefc08844e037d16ef2e8000b5471","source":{"kind":"arxiv","id":"1405.1372","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1405.1372","created_at":"2026-05-18T01:43:17Z"},{"alias_kind":"arxiv_version","alias_value":"1405.1372v1","created_at":"2026-05-18T01:43:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.1372","created_at":"2026-05-18T01:43:17Z"},{"alias_kind":"pith_short_12","alias_value":"6OZA4HANAT3O","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6OZA4HANAT3OKN4R","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6OZA4HAN","created_at":"2026-05-18T12:28:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:6OZA4HANAT3OKN4RBEXJ2SNROT","target":"record","payload":{"canonical_record":{"source":{"id":"1405.1372","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2014-05-06T17:27:11Z","cross_cats_sorted":[],"title_canon_sha256":"54ff0caf6204ef76d32550faae09e8710ee3225ba5c24f17b68302190282ec09","abstract_canon_sha256":"3e9ebb22a61a0cc762e017d9e1f28cf2254748c0a6232be9da44bae539007d4e"},"schema_version":"1.0"},"canonical_sha256":"f3b20e1c0d04f6e53791092e9d49b174d48eefc08844e037d16ef2e8000b5471","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:43:17.115100Z","signature_b64":"cqfWP83g4mFUb8A6PYBmQGh0Wx7GN056rD8tlzlED5S784tlxfZBVC3wZ1KvH1WOanGp/0IkXjsnz5kJie5wDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f3b20e1c0d04f6e53791092e9d49b174d48eefc08844e037d16ef2e8000b5471","last_reissued_at":"2026-05-18T01:43:17.114452Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:43:17.114452Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1405.1372","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":"2026-05-18T01:43:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cZ+dQBebgCCBYz7EfzIZAb+v7hNAAVJMSbWYOKilsoS9heDc/hTdTt4lnMOFsctPSsGRb/2av2JIJwkoQxSQBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T19:05:35.933546Z"},"content_sha256":"0d11004afd066bd2c17250cfb176996268751c9ce23ea90d91d6488ccca853b9","schema_version":"1.0","event_id":"sha256:0d11004afd066bd2c17250cfb176996268751c9ce23ea90d91d6488ccca853b9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:6OZA4HANAT3OKN4RBEXJ2SNROT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Near-wall nanovelocimetry based on Total Internal Reflection Fluorescence with continuous tracking","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Benjamin Chollet, Bruno Bresson, Choongyeop Lee, Fabrice Monti, Lo\\\"ic D'eramo, Marc Yonger, Patrick Tabeling, Yvette Tran, Zhenzhen Li","submitted_at":"2014-05-06T17:27:11Z","abstract_excerpt":"The goal of this work is to make progress in the domain of near-wall velocimetry. The technique we use is based on the tracking of nanoparticles in an evanescent field, close to a wall, a technique called TIRF (Total Internal Reflection Fluorescence)-based velocimetry. At variance with the methods developed in the literature, we permanently keep track of the light emitted by each particle during the time the measurements of their positions ('altitudes') and speeds are performed. By performing the Langevin simulation, we quantified effect of biases such as Brownian motion, heterogeneities induc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.1372","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":"2026-05-18T01:43:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Au4lT2pQjxGq6kPet89ja0SHxTjAYCwPRp8Wccr85aJohYDfiUJsqoET4tGBDAj37h7lKEKuM/fBdYnjDaGlCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T19:05:35.933901Z"},"content_sha256":"2e6b1d0be6cfde76419015f4e99fed0efef2ee22f1cd677bcd9cbbb5601de383","schema_version":"1.0","event_id":"sha256:2e6b1d0be6cfde76419015f4e99fed0efef2ee22f1cd677bcd9cbbb5601de383"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6OZA4HANAT3OKN4RBEXJ2SNROT/bundle.json","state_url":"https://pith.science/pith/6OZA4HANAT3OKN4RBEXJ2SNROT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6OZA4HANAT3OKN4RBEXJ2SNROT/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":"2026-06-06T19:05:35Z","links":{"resolver":"https://pith.science/pith/6OZA4HANAT3OKN4RBEXJ2SNROT","bundle":"https://pith.science/pith/6OZA4HANAT3OKN4RBEXJ2SNROT/bundle.json","state":"https://pith.science/pith/6OZA4HANAT3OKN4RBEXJ2SNROT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6OZA4HANAT3OKN4RBEXJ2SNROT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:6OZA4HANAT3OKN4RBEXJ2SNROT","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":"3e9ebb22a61a0cc762e017d9e1f28cf2254748c0a6232be9da44bae539007d4e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2014-05-06T17:27:11Z","title_canon_sha256":"54ff0caf6204ef76d32550faae09e8710ee3225ba5c24f17b68302190282ec09"},"schema_version":"1.0","source":{"id":"1405.1372","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1405.1372","created_at":"2026-05-18T01:43:17Z"},{"alias_kind":"arxiv_version","alias_value":"1405.1372v1","created_at":"2026-05-18T01:43:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.1372","created_at":"2026-05-18T01:43:17Z"},{"alias_kind":"pith_short_12","alias_value":"6OZA4HANAT3O","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6OZA4HANAT3OKN4R","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6OZA4HAN","created_at":"2026-05-18T12:28:16Z"}],"graph_snapshots":[{"event_id":"sha256:2e6b1d0be6cfde76419015f4e99fed0efef2ee22f1cd677bcd9cbbb5601de383","target":"graph","created_at":"2026-05-18T01:43:17Z","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 goal of this work is to make progress in the domain of near-wall velocimetry. The technique we use is based on the tracking of nanoparticles in an evanescent field, close to a wall, a technique called TIRF (Total Internal Reflection Fluorescence)-based velocimetry. At variance with the methods developed in the literature, we permanently keep track of the light emitted by each particle during the time the measurements of their positions ('altitudes') and speeds are performed. By performing the Langevin simulation, we quantified effect of biases such as Brownian motion, heterogeneities induc","authors_text":"Benjamin Chollet, Bruno Bresson, Choongyeop Lee, Fabrice Monti, Lo\\\"ic D'eramo, Marc Yonger, Patrick Tabeling, Yvette Tran, Zhenzhen Li","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2014-05-06T17:27:11Z","title":"Near-wall nanovelocimetry based on Total Internal Reflection Fluorescence with continuous tracking"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.1372","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":"sha256:0d11004afd066bd2c17250cfb176996268751c9ce23ea90d91d6488ccca853b9","target":"record","created_at":"2026-05-18T01:43:17Z","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":"3e9ebb22a61a0cc762e017d9e1f28cf2254748c0a6232be9da44bae539007d4e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2014-05-06T17:27:11Z","title_canon_sha256":"54ff0caf6204ef76d32550faae09e8710ee3225ba5c24f17b68302190282ec09"},"schema_version":"1.0","source":{"id":"1405.1372","kind":"arxiv","version":1}},"canonical_sha256":"f3b20e1c0d04f6e53791092e9d49b174d48eefc08844e037d16ef2e8000b5471","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f3b20e1c0d04f6e53791092e9d49b174d48eefc08844e037d16ef2e8000b5471","first_computed_at":"2026-05-18T01:43:17.114452Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:43:17.114452Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"cqfWP83g4mFUb8A6PYBmQGh0Wx7GN056rD8tlzlED5S784tlxfZBVC3wZ1KvH1WOanGp/0IkXjsnz5kJie5wDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:43:17.115100Z","signed_message":"canonical_sha256_bytes"},"source_id":"1405.1372","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0d11004afd066bd2c17250cfb176996268751c9ce23ea90d91d6488ccca853b9","sha256:2e6b1d0be6cfde76419015f4e99fed0efef2ee22f1cd677bcd9cbbb5601de383"],"state_sha256":"67fe806c23a95327a5ad8a399cc65f27822a16485ce6bf1c9c3687b82c9e91be"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fpXIzDQbmMDoeQzGKq84/+dCb7yG8tV6j3ziTotL0sX0GSIa4IaeiT26mY8LBkGVn0jFADiRxc1eX7Ss/z3cDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T19:05:35.935754Z","bundle_sha256":"17374fb3388554cd5d022c782205bce415f7790d52204869e6a4c4afa54c5881"}}