{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:ZTZS5SKFETLODC2YP66FFJDGTZ","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":"40d576621720ca65772b4f74223f2081139fbf1d9275b7715b193c6a05315eee","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","physics.gen-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2009-05-19T22:43:24Z","title_canon_sha256":"bef9b52db785e90dfb6adaea25d907d007f9301238161c0d20fed67d70616951"},"schema_version":"1.0","source":{"id":"0905.3196","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0905.3196","created_at":"2026-05-18T02:13:38Z"},{"alias_kind":"arxiv_version","alias_value":"0905.3196v1","created_at":"2026-05-18T02:13:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0905.3196","created_at":"2026-05-18T02:13:38Z"},{"alias_kind":"pith_short_12","alias_value":"ZTZS5SKFETLO","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_16","alias_value":"ZTZS5SKFETLODC2Y","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_8","alias_value":"ZTZS5SKF","created_at":"2026-05-18T12:26:03Z"}],"graph_snapshots":[{"event_id":"sha256:2ef49c82f55542706b964aee5517e542b069b02a82dea343d124ab25ae46b602","target":"graph","created_at":"2026-05-18T02:13:38Z","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":"Real data are constrained to finite sampling rates, which calls for a suitable mathematical description of the corrections to the finite-time estimations of the dynamic equations. Often in the literature, lower order discrete time approximations of the modeling diffusion processes are considered. On the other hand, there is a lack of simple estimating procedures based on higher order approximations. For standard diffusion models, that include additive and multiplicative noise components, we obtain the exact corrections to the empirical finite-time drift and diffusion coefficients, based on It\\","authors_text":"C. Anteneodo, R. Riera","cross_cats":["cond-mat.stat-mech","math-ph","math.MP","physics.gen-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2009-05-19T22:43:24Z","title":"Exact corrections for finite-time drift and diffusion coefficients"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0905.3196","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:d19837df6c744da38937f5d469196f279b4f5e94c4bf3b4255aa5721937c1139","target":"record","created_at":"2026-05-18T02:13:38Z","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":"40d576621720ca65772b4f74223f2081139fbf1d9275b7715b193c6a05315eee","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","physics.gen-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.data-an","submitted_at":"2009-05-19T22:43:24Z","title_canon_sha256":"bef9b52db785e90dfb6adaea25d907d007f9301238161c0d20fed67d70616951"},"schema_version":"1.0","source":{"id":"0905.3196","kind":"arxiv","version":1}},"canonical_sha256":"ccf32ec94524d6e18b587fbc52a4669e7d75f8ad712fc66c66f65fdb16b5f143","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ccf32ec94524d6e18b587fbc52a4669e7d75f8ad712fc66c66f65fdb16b5f143","first_computed_at":"2026-05-18T02:13:38.512459Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:13:38.512459Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"XxD/z23WaaME7f0p5LttGySWMbaK0ap8nTCLQQNX4MHp6pxt4LkgWBEqjLjrRsRIANa2tEiEEL0y09atEvhuAg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:13:38.512924Z","signed_message":"canonical_sha256_bytes"},"source_id":"0905.3196","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d19837df6c744da38937f5d469196f279b4f5e94c4bf3b4255aa5721937c1139","sha256:2ef49c82f55542706b964aee5517e542b069b02a82dea343d124ab25ae46b602"],"state_sha256":"6607511816e01f39d65cd9d365bb12b2e3c56ab78e5a1d35f0101ec584c457a5"}