{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:KXL6WWIAITTMGEVQY25RB77JVU","short_pith_number":"pith:KXL6WWIA","canonical_record":{"source":{"id":"1703.03764","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-10T17:02:41Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"409baf8add17ed2305d6b2513538a82e4d4d07a85964415cb173b2ffa67a6baa","abstract_canon_sha256":"90ceae0a620cacba2dced47e86aa4ae99e8488424c973287017e50475374e83a"},"schema_version":"1.0"},"canonical_sha256":"55d7eb590044e6c312b0c6bb10ffe9ad28ae11dc81a031dc6b808be32bc3c304","source":{"kind":"arxiv","id":"1703.03764","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.03764","created_at":"2026-05-18T00:41:24Z"},{"alias_kind":"arxiv_version","alias_value":"1703.03764v1","created_at":"2026-05-18T00:41:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.03764","created_at":"2026-05-18T00:41:24Z"},{"alias_kind":"pith_short_12","alias_value":"KXL6WWIAITTM","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"KXL6WWIAITTMGEVQ","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"KXL6WWIA","created_at":"2026-05-18T12:31:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:KXL6WWIAITTMGEVQY25RB77JVU","target":"record","payload":{"canonical_record":{"source":{"id":"1703.03764","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-10T17:02:41Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"409baf8add17ed2305d6b2513538a82e4d4d07a85964415cb173b2ffa67a6baa","abstract_canon_sha256":"90ceae0a620cacba2dced47e86aa4ae99e8488424c973287017e50475374e83a"},"schema_version":"1.0"},"canonical_sha256":"55d7eb590044e6c312b0c6bb10ffe9ad28ae11dc81a031dc6b808be32bc3c304","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:41:24.619281Z","signature_b64":"M/17yZlI/o+TN1xjJshvheGbZffJBiowuA+MsVWWtDxZgBfZltj9ZEwcAB9tGuZcl1D+oWckDk0b7Te5ql4yBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"55d7eb590044e6c312b0c6bb10ffe9ad28ae11dc81a031dc6b808be32bc3c304","last_reissued_at":"2026-05-18T00:41:24.618567Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:41:24.618567Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1703.03764","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:41:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2EluEaDo0/RxaPNcdN/lWuQfW63SW8AQdhM8yke8gYDBaipwEFV+2VjBnVpQ2j6pA0ktdDhVC0u975fLSZrGCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:40:54.911041Z"},"content_sha256":"2b54e4075f2242a982fdd01c8467dc83ef2428ac0f90cceeb8315f8b98e67af0","schema_version":"1.0","event_id":"sha256:2b54e4075f2242a982fdd01c8467dc83ef2428ac0f90cceeb8315f8b98e67af0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:KXL6WWIAITTMGEVQY25RB77JVU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Entropy production and time-asymmetry in the presence of strong interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Harry J. D. Miller, Janet Anders","submitted_at":"2017-03-10T17:02:41Z","abstract_excerpt":"It is known that the equilibrium properties of open classical systems that are strongly coupled to a heat bath are described by a set of thermodynamic potentials related to the system's Hamiltonian of mean force. By adapting this framework to a more general class of non-equilibrium states, we show that the equilibrium properties of the bath can be well-defined, even when the system is arbitrarily far from equilibrium and correlated with the bath. These states, which retain a notion of temperature, take the form of conditional equilibrium distributions. For out-of-equilibrium processes we show "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.03764","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:41:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yGMkq7qthgMd3sxCDDkQ6scLu3GehE77S8Ku5DWtxohru0GJ5XvL/0L/iamWPxcfy/t7xVJbW3aYYNE2wuqHCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:40:54.911763Z"},"content_sha256":"9d89f85dc96f9599f9585265ea24425e9456425732146be10f33f10569d60ab9","schema_version":"1.0","event_id":"sha256:9d89f85dc96f9599f9585265ea24425e9456425732146be10f33f10569d60ab9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KXL6WWIAITTMGEVQY25RB77JVU/bundle.json","state_url":"https://pith.science/pith/KXL6WWIAITTMGEVQY25RB77JVU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KXL6WWIAITTMGEVQY25RB77JVU/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":"2026-05-31T15:40:54Z","links":{"resolver":"https://pith.science/pith/KXL6WWIAITTMGEVQY25RB77JVU","bundle":"https://pith.science/pith/KXL6WWIAITTMGEVQY25RB77JVU/bundle.json","state":"https://pith.science/pith/KXL6WWIAITTMGEVQY25RB77JVU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KXL6WWIAITTMGEVQY25RB77JVU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:KXL6WWIAITTMGEVQY25RB77JVU","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":"90ceae0a620cacba2dced47e86aa4ae99e8488424c973287017e50475374e83a","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-10T17:02:41Z","title_canon_sha256":"409baf8add17ed2305d6b2513538a82e4d4d07a85964415cb173b2ffa67a6baa"},"schema_version":"1.0","source":{"id":"1703.03764","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.03764","created_at":"2026-05-18T00:41:24Z"},{"alias_kind":"arxiv_version","alias_value":"1703.03764v1","created_at":"2026-05-18T00:41:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.03764","created_at":"2026-05-18T00:41:24Z"},{"alias_kind":"pith_short_12","alias_value":"KXL6WWIAITTM","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"KXL6WWIAITTMGEVQ","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"KXL6WWIA","created_at":"2026-05-18T12:31:28Z"}],"graph_snapshots":[{"event_id":"sha256:9d89f85dc96f9599f9585265ea24425e9456425732146be10f33f10569d60ab9","target":"graph","created_at":"2026-05-18T00:41:24Z","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":"It is known that the equilibrium properties of open classical systems that are strongly coupled to a heat bath are described by a set of thermodynamic potentials related to the system's Hamiltonian of mean force. By adapting this framework to a more general class of non-equilibrium states, we show that the equilibrium properties of the bath can be well-defined, even when the system is arbitrarily far from equilibrium and correlated with the bath. These states, which retain a notion of temperature, take the form of conditional equilibrium distributions. For out-of-equilibrium processes we show ","authors_text":"Harry J. D. Miller, Janet Anders","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-10T17:02:41Z","title":"Entropy production and time-asymmetry in the presence of strong interactions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.03764","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":"sha256:2b54e4075f2242a982fdd01c8467dc83ef2428ac0f90cceeb8315f8b98e67af0","target":"record","created_at":"2026-05-18T00:41:24Z","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":"90ceae0a620cacba2dced47e86aa4ae99e8488424c973287017e50475374e83a","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-10T17:02:41Z","title_canon_sha256":"409baf8add17ed2305d6b2513538a82e4d4d07a85964415cb173b2ffa67a6baa"},"schema_version":"1.0","source":{"id":"1703.03764","kind":"arxiv","version":1}},"canonical_sha256":"55d7eb590044e6c312b0c6bb10ffe9ad28ae11dc81a031dc6b808be32bc3c304","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"55d7eb590044e6c312b0c6bb10ffe9ad28ae11dc81a031dc6b808be32bc3c304","first_computed_at":"2026-05-18T00:41:24.618567Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:41:24.618567Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"M/17yZlI/o+TN1xjJshvheGbZffJBiowuA+MsVWWtDxZgBfZltj9ZEwcAB9tGuZcl1D+oWckDk0b7Te5ql4yBA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:41:24.619281Z","signed_message":"canonical_sha256_bytes"},"source_id":"1703.03764","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2b54e4075f2242a982fdd01c8467dc83ef2428ac0f90cceeb8315f8b98e67af0","sha256:9d89f85dc96f9599f9585265ea24425e9456425732146be10f33f10569d60ab9"],"state_sha256":"6af03132a1f9a393fec5506d030d0525e7a73c69b0c3b4ecb6ab552ab8a5bd42"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9fib0skn0Oh1bW33olkb/DKiqU0wIfkmO+nFCMNRBwPmfFGC557kvy0Jet0XmhboG8ksYpQ5e8y78Hwff9VVDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T15:40:54.915257Z","bundle_sha256":"abfa754bd2b8180d2282ffe791666b55117c55b39d3d87e97d72ba6f1fc6b8fc"}}