{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:DQEIJOGMSY2ILRHIQV2LB2WLUF","short_pith_number":"pith:DQEIJOGM","schema_version":"1.0","canonical_sha256":"1c0884b8cc963485c4e88574b0eacba14370643fbeec42ab5928f9266863cc5b","source":{"kind":"arxiv","id":"1708.07032","version":2},"attestation_state":"computed","paper":{"title":"Discrete-time thermodynamic uncertainty relation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Christian Van den Broeck, Karel Proesmans","submitted_at":"2017-08-23T14:55:14Z","abstract_excerpt":"We generalize the thermodynamic uncertainty relation, providing an entropic upper bound for average fluxes in time-continuous steady-state systems (Gingrich et al., Phys. Rev. Lett. 116, 120601 (2016)), to time-discrete Markov chains and to systems under time-symmetric, periodic driving."},"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":"1708.07032","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-08-23T14:55:14Z","cross_cats_sorted":[],"title_canon_sha256":"b81e0ebc5aa869f4263948aae30d8312c398dd4dddeb96d0b813a846ce86a146","abstract_canon_sha256":"e51747bc387bac00603a3cbe0ce8e796367ec5b73e37c216303e82af10aac056"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:15.660725Z","signature_b64":"pDswJakU3rq1XAL3h+7n11ZhCNcEb555myKpzjwxEWA2iN5YYws7ln3ZvO9nDjf04s42Heenu7K0sodPjmrgDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1c0884b8cc963485c4e88574b0eacba14370643fbeec42ab5928f9266863cc5b","last_reissued_at":"2026-05-18T00:33:15.660086Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:15.660086Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Discrete-time thermodynamic uncertainty relation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Christian Van den Broeck, Karel Proesmans","submitted_at":"2017-08-23T14:55:14Z","abstract_excerpt":"We generalize the thermodynamic uncertainty relation, providing an entropic upper bound for average fluxes in time-continuous steady-state systems (Gingrich et al., Phys. Rev. Lett. 116, 120601 (2016)), to time-discrete Markov chains and to systems under time-symmetric, periodic driving."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.07032","kind":"arxiv","version":2},"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":"1708.07032","created_at":"2026-05-18T00:33:15.660171+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.07032v2","created_at":"2026-05-18T00:33:15.660171+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.07032","created_at":"2026-05-18T00:33:15.660171+00:00"},{"alias_kind":"pith_short_12","alias_value":"DQEIJOGMSY2I","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_16","alias_value":"DQEIJOGMSY2ILRHI","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_8","alias_value":"DQEIJOGM","created_at":"2026-05-18T12:31:12.930513+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/DQEIJOGMSY2ILRHIQV2LB2WLUF","json":"https://pith.science/pith/DQEIJOGMSY2ILRHIQV2LB2WLUF.json","graph_json":"https://pith.science/api/pith-number/DQEIJOGMSY2ILRHIQV2LB2WLUF/graph.json","events_json":"https://pith.science/api/pith-number/DQEIJOGMSY2ILRHIQV2LB2WLUF/events.json","paper":"https://pith.science/paper/DQEIJOGM"},"agent_actions":{"view_html":"https://pith.science/pith/DQEIJOGMSY2ILRHIQV2LB2WLUF","download_json":"https://pith.science/pith/DQEIJOGMSY2ILRHIQV2LB2WLUF.json","view_paper":"https://pith.science/paper/DQEIJOGM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.07032&json=true","fetch_graph":"https://pith.science/api/pith-number/DQEIJOGMSY2ILRHIQV2LB2WLUF/graph.json","fetch_events":"https://pith.science/api/pith-number/DQEIJOGMSY2ILRHIQV2LB2WLUF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DQEIJOGMSY2ILRHIQV2LB2WLUF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DQEIJOGMSY2ILRHIQV2LB2WLUF/action/storage_attestation","attest_author":"https://pith.science/pith/DQEIJOGMSY2ILRHIQV2LB2WLUF/action/author_attestation","sign_citation":"https://pith.science/pith/DQEIJOGMSY2ILRHIQV2LB2WLUF/action/citation_signature","submit_replication":"https://pith.science/pith/DQEIJOGMSY2ILRHIQV2LB2WLUF/action/replication_record"}},"created_at":"2026-05-18T00:33:15.660171+00:00","updated_at":"2026-05-18T00:33:15.660171+00:00"}