{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:Z3RV2TBSIXLZAYQYZZWQPIIEO6","short_pith_number":"pith:Z3RV2TBS","schema_version":"1.0","canonical_sha256":"cee35d4c3245d7906218ce6d07a10477ac896546e9e224460be8b595dccb9252","source":{"kind":"arxiv","id":"1102.3938","version":1},"attestation_state":"computed","paper":{"title":"Large-deviation principles, stochastic effective actions, path entropies, and the structure and meaning of thermodynamic descriptions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"cond-mat.stat-mech","authors_text":"Eric Smith","submitted_at":"2011-02-18T23:40:48Z","abstract_excerpt":"The meaning of thermodynamic descriptions is found in large-deviations scaling of the fluctuations probabilities. The primary large-deviations rate function is the entropy, which is the basis for both fluctuation theorems and for characterizing the thermodynamic interactions of systems. Freidlin-Wentzell theory provides a general formulation of large-deviations scaling for non-equilibrium stochastic processes, through a representation in terms of a Hamiltonian dynamical system. A number of related methods now exist to construct the Freidlin-Wentzell Hamiltonian for many kinds of stochastic pro"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1102.3938","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-02-18T23:40:48Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"ad4aa24d5de52b2979590350e0fb0bf8ab6ff33708cbc18dcf6d40ce4344e5ae","abstract_canon_sha256":"ad5044350c833001a9409413603e743daa821a78908d1488c7bb2431bcf03c22"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:03:07.606672Z","signature_b64":"rI5BTf2g72UrE6/2zR8LSKPl8Jajo8EKFv1EA/wG2GgWbchOPCanboCCu6qwCLiDbvams5xoW7rRGQZ4ZDVGAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cee35d4c3245d7906218ce6d07a10477ac896546e9e224460be8b595dccb9252","last_reissued_at":"2026-05-18T02:03:07.606264Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:03:07.606264Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Large-deviation principles, stochastic effective actions, path entropies, and the structure and meaning of thermodynamic descriptions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"cond-mat.stat-mech","authors_text":"Eric Smith","submitted_at":"2011-02-18T23:40:48Z","abstract_excerpt":"The meaning of thermodynamic descriptions is found in large-deviations scaling of the fluctuations probabilities. The primary large-deviations rate function is the entropy, which is the basis for both fluctuation theorems and for characterizing the thermodynamic interactions of systems. Freidlin-Wentzell theory provides a general formulation of large-deviations scaling for non-equilibrium stochastic processes, through a representation in terms of a Hamiltonian dynamical system. A number of related methods now exist to construct the Freidlin-Wentzell Hamiltonian for many kinds of stochastic pro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1102.3938","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1102.3938","created_at":"2026-05-18T02:03:07.606327+00:00"},{"alias_kind":"arxiv_version","alias_value":"1102.3938v1","created_at":"2026-05-18T02:03:07.606327+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1102.3938","created_at":"2026-05-18T02:03:07.606327+00:00"},{"alias_kind":"pith_short_12","alias_value":"Z3RV2TBSIXLZ","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_16","alias_value":"Z3RV2TBSIXLZAYQY","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_8","alias_value":"Z3RV2TBS","created_at":"2026-05-18T12:26:47.523578+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Z3RV2TBSIXLZAYQYZZWQPIIEO6","json":"https://pith.science/pith/Z3RV2TBSIXLZAYQYZZWQPIIEO6.json","graph_json":"https://pith.science/api/pith-number/Z3RV2TBSIXLZAYQYZZWQPIIEO6/graph.json","events_json":"https://pith.science/api/pith-number/Z3RV2TBSIXLZAYQYZZWQPIIEO6/events.json","paper":"https://pith.science/paper/Z3RV2TBS"},"agent_actions":{"view_html":"https://pith.science/pith/Z3RV2TBSIXLZAYQYZZWQPIIEO6","download_json":"https://pith.science/pith/Z3RV2TBSIXLZAYQYZZWQPIIEO6.json","view_paper":"https://pith.science/paper/Z3RV2TBS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1102.3938&json=true","fetch_graph":"https://pith.science/api/pith-number/Z3RV2TBSIXLZAYQYZZWQPIIEO6/graph.json","fetch_events":"https://pith.science/api/pith-number/Z3RV2TBSIXLZAYQYZZWQPIIEO6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Z3RV2TBSIXLZAYQYZZWQPIIEO6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Z3RV2TBSIXLZAYQYZZWQPIIEO6/action/storage_attestation","attest_author":"https://pith.science/pith/Z3RV2TBSIXLZAYQYZZWQPIIEO6/action/author_attestation","sign_citation":"https://pith.science/pith/Z3RV2TBSIXLZAYQYZZWQPIIEO6/action/citation_signature","submit_replication":"https://pith.science/pith/Z3RV2TBSIXLZAYQYZZWQPIIEO6/action/replication_record"}},"created_at":"2026-05-18T02:03:07.606327+00:00","updated_at":"2026-05-18T02:03:07.606327+00:00"}