{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:57PUWZPZ6K5DTV3W4NPTOXTCPC","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":"c851fbc2e4c9ec6c5112c884f09b260b296e1c34f122e7a2912729627bbd998b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2019-08-15T14:23:48Z","title_canon_sha256":"3c0eb86e12095e6c80aaa933216047e753e2184fefe02f7351b33303f84af0a4"},"schema_version":"1.0","source":{"id":"1908.05560","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1908.05560","created_at":"2026-07-05T01:37:52Z"},{"alias_kind":"arxiv_version","alias_value":"1908.05560v1","created_at":"2026-07-05T01:37:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.05560","created_at":"2026-07-05T01:37:52Z"},{"alias_kind":"pith_short_12","alias_value":"57PUWZPZ6K5D","created_at":"2026-07-05T01:37:52Z"},{"alias_kind":"pith_short_16","alias_value":"57PUWZPZ6K5DTV3W","created_at":"2026-07-05T01:37:52Z"},{"alias_kind":"pith_short_8","alias_value":"57PUWZPZ","created_at":"2026-07-05T01:37:52Z"}],"graph_snapshots":[{"event_id":"sha256:9a29e1040bd1954f84a09d8a4d3e81285d3addaad797063f942b89eabcbf78d9","target":"graph","created_at":"2026-07-05T01:37:52Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/1908.05560/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We introduce a field-theoretic thermodynamic uncertainty relation as an extension of the one derived so far for a Markovian dynamics on a discrete set of states and for overdamped Langevin equations. We first formulate a framework which describes quantities like current, entropy production and diffusivity in the case of a generic field theory. We will then apply this general setting to the one-dimensional Kardar-Parisi-Zhang equation, a paradigmatic example of a non-linear field-theoretic Langevin equation. In particular, we will treat the dimensionless Kardar-Parisi-Zhang equation with an eff","authors_text":"Oliver Niggemann, Udo Seifert","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2019-08-15T14:23:48Z","title":"Field-Theoretic Thermodynamic Uncertainty Relation -- General formulation exemplified with the Kardar-Parisi-Zhang equation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.05560","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":"sha256:0bc866247be7874cd8fdae0c90b125f122f42494424533cc6d1c239d88a383e6","target":"record","created_at":"2026-07-05T01:37:52Z","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":"c851fbc2e4c9ec6c5112c884f09b260b296e1c34f122e7a2912729627bbd998b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2019-08-15T14:23:48Z","title_canon_sha256":"3c0eb86e12095e6c80aaa933216047e753e2184fefe02f7351b33303f84af0a4"},"schema_version":"1.0","source":{"id":"1908.05560","kind":"arxiv","version":1}},"canonical_sha256":"efdf4b65f9f2ba39d776e35f375e6278a8d03c0517034324f6af21cdbf94c360","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"efdf4b65f9f2ba39d776e35f375e6278a8d03c0517034324f6af21cdbf94c360","first_computed_at":"2026-07-05T01:37:52.171526Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:37:52.171526Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"h0LMgEA/mDHyH1fVH1WqvUPZT4UPhjhDiuVw8tOA7qaxoWQcYBN6DJwpEcUvarBOOSnwhL4OgZk9ANkE6HaGAg==","signature_status":"signed_v1","signed_at":"2026-07-05T01:37:52.171912Z","signed_message":"canonical_sha256_bytes"},"source_id":"1908.05560","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0bc866247be7874cd8fdae0c90b125f122f42494424533cc6d1c239d88a383e6","sha256:9a29e1040bd1954f84a09d8a4d3e81285d3addaad797063f942b89eabcbf78d9"],"state_sha256":"85274e097cdfdf45c78cf3b0db8defba393733b7669ff4110c969a179c10e756"}