{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:27XG42M5YVVEXTXSUNXJCSQ52H","short_pith_number":"pith:27XG42M5","canonical_record":{"source":{"id":"2303.16337","kind":"arxiv","version":5},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-03-28T22:27:22Z","cross_cats_sorted":[],"title_canon_sha256":"65ac64e98ba046405a171e1e6c95820706cc42f9e28894812afb9c1d0d760092","abstract_canon_sha256":"1798c9228e75416adc562bb8cd3f46e7a3d46d8f75e155642f6b040a37cae294"},"schema_version":"1.0"},"canonical_sha256":"d7ee6e699dc56a4bcef2a36e914a1dd1d412baa9e669b5da7456d6e544842597","source":{"kind":"arxiv","id":"2303.16337","version":5},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2303.16337","created_at":"2026-07-05T10:14:01Z"},{"alias_kind":"arxiv_version","alias_value":"2303.16337v5","created_at":"2026-07-05T10:14:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2303.16337","created_at":"2026-07-05T10:14:01Z"},{"alias_kind":"pith_short_12","alias_value":"27XG42M5YVVE","created_at":"2026-07-05T10:14:01Z"},{"alias_kind":"pith_short_16","alias_value":"27XG42M5YVVEXTXS","created_at":"2026-07-05T10:14:01Z"},{"alias_kind":"pith_short_8","alias_value":"27XG42M5","created_at":"2026-07-05T10:14:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:27XG42M5YVVEXTXSUNXJCSQ52H","target":"record","payload":{"canonical_record":{"source":{"id":"2303.16337","kind":"arxiv","version":5},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-03-28T22:27:22Z","cross_cats_sorted":[],"title_canon_sha256":"65ac64e98ba046405a171e1e6c95820706cc42f9e28894812afb9c1d0d760092","abstract_canon_sha256":"1798c9228e75416adc562bb8cd3f46e7a3d46d8f75e155642f6b040a37cae294"},"schema_version":"1.0"},"canonical_sha256":"d7ee6e699dc56a4bcef2a36e914a1dd1d412baa9e669b5da7456d6e544842597","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:14:01.268406Z","signature_b64":"0n0Hm2Y1P6moYzkg2NMMokAG/wfyjhfa6VJphZLiljMRlaXHJmUMFZvnZyUIEk3WmGpI0ytFxxtSLBCaF/+1CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d7ee6e699dc56a4bcef2a36e914a1dd1d412baa9e669b5da7456d6e544842597","last_reissued_at":"2026-07-05T10:14:01.267940Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:14:01.267940Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2303.16337","source_version":5,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T10:14:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qGskKRPcX9X2jqxA5HTkKSFDdi/0PCpbaDy8T8RluZasVTl/k/LMqWUCC7pg5ck9Jv2LFJIpts2YsGIhcfvdCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-09T06:54:18.478687Z"},"content_sha256":"c7ed86185208596bafebcbb8d0796d7cd50d94b9bfa0d59b1c08ad99667b9cdb","schema_version":"1.0","event_id":"sha256:c7ed86185208596bafebcbb8d0796d7cd50d94b9bfa0d59b1c08ad99667b9cdb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:27XG42M5YVVEXTXSUNXJCSQ52H","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fluctuation theorems for quasistatic work","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Pierre Naz\\'e","submitted_at":"2023-03-28T22:27:22Z","abstract_excerpt":"When a thermally isolated system performs a driving process in the quasistatic regime, its variation of average energy is equal to its quasistatic work. Even though presenting this simple definition, few attempts have been made to describe such quantity from the fluctuation theorem point of view. In this work, based on Jarzynski's equality, four forms of such equality are deduced. To corroborate the result, a relation with the strong inequality $\\langle W\\rangle\\ge \\langle W_{\\rm qs}\\rangle$ is pursued. It is concluded in the end that any of the fluctuation theorems deduced cannot derive such "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.16337","kind":"arxiv","version":5},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2303.16337/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T10:14:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pdMqhDf2cAp0KvIBgmrQlalNtRDO9ivf5WDsa4Gt1pFUEOA75kANthBirQ5dEiJXC46nXBfbkvD+5vMdQhg9AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-09T06:54:18.479083Z"},"content_sha256":"a209bea020fb7d192db416c4997f6934db708da779d4b756a0c9e9a4bdf5954e","schema_version":"1.0","event_id":"sha256:a209bea020fb7d192db416c4997f6934db708da779d4b756a0c9e9a4bdf5954e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/27XG42M5YVVEXTXSUNXJCSQ52H/bundle.json","state_url":"https://pith.science/pith/27XG42M5YVVEXTXSUNXJCSQ52H/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/27XG42M5YVVEXTXSUNXJCSQ52H/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":"2026-07-09T06:54:18Z","links":{"resolver":"https://pith.science/pith/27XG42M5YVVEXTXSUNXJCSQ52H","bundle":"https://pith.science/pith/27XG42M5YVVEXTXSUNXJCSQ52H/bundle.json","state":"https://pith.science/pith/27XG42M5YVVEXTXSUNXJCSQ52H/state.json","well_known_bundle":"https://pith.science/.well-known/pith/27XG42M5YVVEXTXSUNXJCSQ52H/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:27XG42M5YVVEXTXSUNXJCSQ52H","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":"1798c9228e75416adc562bb8cd3f46e7a3d46d8f75e155642f6b040a37cae294","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-03-28T22:27:22Z","title_canon_sha256":"65ac64e98ba046405a171e1e6c95820706cc42f9e28894812afb9c1d0d760092"},"schema_version":"1.0","source":{"id":"2303.16337","kind":"arxiv","version":5}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2303.16337","created_at":"2026-07-05T10:14:01Z"},{"alias_kind":"arxiv_version","alias_value":"2303.16337v5","created_at":"2026-07-05T10:14:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2303.16337","created_at":"2026-07-05T10:14:01Z"},{"alias_kind":"pith_short_12","alias_value":"27XG42M5YVVE","created_at":"2026-07-05T10:14:01Z"},{"alias_kind":"pith_short_16","alias_value":"27XG42M5YVVEXTXS","created_at":"2026-07-05T10:14:01Z"},{"alias_kind":"pith_short_8","alias_value":"27XG42M5","created_at":"2026-07-05T10:14:01Z"}],"graph_snapshots":[{"event_id":"sha256:a209bea020fb7d192db416c4997f6934db708da779d4b756a0c9e9a4bdf5954e","target":"graph","created_at":"2026-07-05T10:14:01Z","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/2303.16337/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"When a thermally isolated system performs a driving process in the quasistatic regime, its variation of average energy is equal to its quasistatic work. Even though presenting this simple definition, few attempts have been made to describe such quantity from the fluctuation theorem point of view. In this work, based on Jarzynski's equality, four forms of such equality are deduced. To corroborate the result, a relation with the strong inequality $\\langle W\\rangle\\ge \\langle W_{\\rm qs}\\rangle$ is pursued. It is concluded in the end that any of the fluctuation theorems deduced cannot derive such ","authors_text":"Pierre Naz\\'e","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-03-28T22:27:22Z","title":"Fluctuation theorems for quasistatic work"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.16337","kind":"arxiv","version":5},"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:c7ed86185208596bafebcbb8d0796d7cd50d94b9bfa0d59b1c08ad99667b9cdb","target":"record","created_at":"2026-07-05T10:14:01Z","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":"1798c9228e75416adc562bb8cd3f46e7a3d46d8f75e155642f6b040a37cae294","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2023-03-28T22:27:22Z","title_canon_sha256":"65ac64e98ba046405a171e1e6c95820706cc42f9e28894812afb9c1d0d760092"},"schema_version":"1.0","source":{"id":"2303.16337","kind":"arxiv","version":5}},"canonical_sha256":"d7ee6e699dc56a4bcef2a36e914a1dd1d412baa9e669b5da7456d6e544842597","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d7ee6e699dc56a4bcef2a36e914a1dd1d412baa9e669b5da7456d6e544842597","first_computed_at":"2026-07-05T10:14:01.267940Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:14:01.267940Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0n0Hm2Y1P6moYzkg2NMMokAG/wfyjhfa6VJphZLiljMRlaXHJmUMFZvnZyUIEk3WmGpI0ytFxxtSLBCaF/+1CQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:14:01.268406Z","signed_message":"canonical_sha256_bytes"},"source_id":"2303.16337","source_kind":"arxiv","source_version":5}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c7ed86185208596bafebcbb8d0796d7cd50d94b9bfa0d59b1c08ad99667b9cdb","sha256:a209bea020fb7d192db416c4997f6934db708da779d4b756a0c9e9a4bdf5954e"],"state_sha256":"847d2f8ee9380c9ce839dbff733587a1be1125057daf12c8cb112f1f1c01f17c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gzvQEGoM9J5t+vdSjB4QaKOWZGNIxwXI2sxR0r7+hOcikbHZfH1zKt5vwtFx+D6I/Otg6aERAz02nu0isdX8Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-09T06:54:18.481971Z","bundle_sha256":"08c2aa4b02dbbb9cb7a1cdc800d940d5264ce7d81067089801f65eab441f1052"}}