{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:WDL4GYPOZPX64QLUTS6XYMVGCP","short_pith_number":"pith:WDL4GYPO","canonical_record":{"source":{"id":"1807.00116","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-06-30T03:09:37Z","cross_cats_sorted":[],"title_canon_sha256":"8f9f99859c9c97b5f93185bba6ee2df890ae7c16b545e95e3597b68f9f21448a","abstract_canon_sha256":"1ff7dabe33cd784ef1b7da9ab0ddf898f807b198b063d6fcdd24b00bd1ba921c"},"schema_version":"1.0"},"canonical_sha256":"b0d7c361eecbefee41749cbd7c32a613fe27c08d4cce24b6301b834af4c32042","source":{"kind":"arxiv","id":"1807.00116","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.00116","created_at":"2026-05-18T00:04:07Z"},{"alias_kind":"arxiv_version","alias_value":"1807.00116v1","created_at":"2026-05-18T00:04:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.00116","created_at":"2026-05-18T00:04:07Z"},{"alias_kind":"pith_short_12","alias_value":"WDL4GYPOZPX6","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_16","alias_value":"WDL4GYPOZPX64QLU","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_8","alias_value":"WDL4GYPO","created_at":"2026-05-18T12:32:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:WDL4GYPOZPX64QLUTS6XYMVGCP","target":"record","payload":{"canonical_record":{"source":{"id":"1807.00116","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-06-30T03:09:37Z","cross_cats_sorted":[],"title_canon_sha256":"8f9f99859c9c97b5f93185bba6ee2df890ae7c16b545e95e3597b68f9f21448a","abstract_canon_sha256":"1ff7dabe33cd784ef1b7da9ab0ddf898f807b198b063d6fcdd24b00bd1ba921c"},"schema_version":"1.0"},"canonical_sha256":"b0d7c361eecbefee41749cbd7c32a613fe27c08d4cce24b6301b834af4c32042","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:07.546327Z","signature_b64":"OcFkT6lv3CaxrXeBTfgkOkNGkVhdiY3OItD+M4e3656Ai17/pq6XvccV5KclXn7c40Nm7f4xV2528LpgowlbBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b0d7c361eecbefee41749cbd7c32a613fe27c08d4cce24b6301b834af4c32042","last_reissued_at":"2026-05-18T00:04:07.545662Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:07.545662Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1807.00116","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":"2026-05-18T00:04:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2CIlGPxiNHWWu9AwFDyJ7vSEkN2I4oJmyTT/kIvhZBTK2Pjdzvb+pttDvijyM6VzPQYKHnjNMbz8SNf9mJYbCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T08:40:15.118646Z"},"content_sha256":"441e52d971bf732d1d8a69bb943ca3ab0c8969d63bae2f90472f65908abdca3b","schema_version":"1.0","event_id":"sha256:441e52d971bf732d1d8a69bb943ca3ab0c8969d63bae2f90472f65908abdca3b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:WDL4GYPOZPX64QLUTS6XYMVGCP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Energy dissipation and information flow in coupled Markovian systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"David A. Sivak, Matthew E. Quenneville","submitted_at":"2018-06-30T03:09:37Z","abstract_excerpt":"A stochastic system under the influence of a stochastic environment is correlated with both present and future states of the environment. Such a system can be seen as implicitly implementing a predictive model of future environmental states. The non-predictive model complexity has been shown to lower-bound the thermodynamic dissipation. Here we explore these statistical and physical quantities at steady state in simple models. We show that under quasi-static driving this model complexity saturates the dissipation. Beyond the quasi-static limit, we demonstrate a lower bound on the ratio of this"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.00116","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":"2026-05-18T00:04:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CHdkxBAt17Wq7Mc9IaauNGG/L1nBP44UXLb2QJx7vmCEESx4BgAWeHSyhgoM27GEU8DsGvpeRED8pL0hakNuDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T08:40:15.119006Z"},"content_sha256":"c114d1ec0d666bbfb0bd945ee9d8f0dbcff07855bf94c8cc2223c40106b60dc0","schema_version":"1.0","event_id":"sha256:c114d1ec0d666bbfb0bd945ee9d8f0dbcff07855bf94c8cc2223c40106b60dc0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WDL4GYPOZPX64QLUTS6XYMVGCP/bundle.json","state_url":"https://pith.science/pith/WDL4GYPOZPX64QLUTS6XYMVGCP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WDL4GYPOZPX64QLUTS6XYMVGCP/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":"2026-05-20T08:40:15Z","links":{"resolver":"https://pith.science/pith/WDL4GYPOZPX64QLUTS6XYMVGCP","bundle":"https://pith.science/pith/WDL4GYPOZPX64QLUTS6XYMVGCP/bundle.json","state":"https://pith.science/pith/WDL4GYPOZPX64QLUTS6XYMVGCP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WDL4GYPOZPX64QLUTS6XYMVGCP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:WDL4GYPOZPX64QLUTS6XYMVGCP","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":"1ff7dabe33cd784ef1b7da9ab0ddf898f807b198b063d6fcdd24b00bd1ba921c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-06-30T03:09:37Z","title_canon_sha256":"8f9f99859c9c97b5f93185bba6ee2df890ae7c16b545e95e3597b68f9f21448a"},"schema_version":"1.0","source":{"id":"1807.00116","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.00116","created_at":"2026-05-18T00:04:07Z"},{"alias_kind":"arxiv_version","alias_value":"1807.00116v1","created_at":"2026-05-18T00:04:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.00116","created_at":"2026-05-18T00:04:07Z"},{"alias_kind":"pith_short_12","alias_value":"WDL4GYPOZPX6","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_16","alias_value":"WDL4GYPOZPX64QLU","created_at":"2026-05-18T12:32:59Z"},{"alias_kind":"pith_short_8","alias_value":"WDL4GYPO","created_at":"2026-05-18T12:32:59Z"}],"graph_snapshots":[{"event_id":"sha256:c114d1ec0d666bbfb0bd945ee9d8f0dbcff07855bf94c8cc2223c40106b60dc0","target":"graph","created_at":"2026-05-18T00:04:07Z","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":"A stochastic system under the influence of a stochastic environment is correlated with both present and future states of the environment. Such a system can be seen as implicitly implementing a predictive model of future environmental states. The non-predictive model complexity has been shown to lower-bound the thermodynamic dissipation. Here we explore these statistical and physical quantities at steady state in simple models. We show that under quasi-static driving this model complexity saturates the dissipation. Beyond the quasi-static limit, we demonstrate a lower bound on the ratio of this","authors_text":"David A. Sivak, Matthew E. Quenneville","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-06-30T03:09:37Z","title":"Energy dissipation and information flow in coupled Markovian systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.00116","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":"sha256:441e52d971bf732d1d8a69bb943ca3ab0c8969d63bae2f90472f65908abdca3b","target":"record","created_at":"2026-05-18T00:04:07Z","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":"1ff7dabe33cd784ef1b7da9ab0ddf898f807b198b063d6fcdd24b00bd1ba921c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-06-30T03:09:37Z","title_canon_sha256":"8f9f99859c9c97b5f93185bba6ee2df890ae7c16b545e95e3597b68f9f21448a"},"schema_version":"1.0","source":{"id":"1807.00116","kind":"arxiv","version":1}},"canonical_sha256":"b0d7c361eecbefee41749cbd7c32a613fe27c08d4cce24b6301b834af4c32042","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b0d7c361eecbefee41749cbd7c32a613fe27c08d4cce24b6301b834af4c32042","first_computed_at":"2026-05-18T00:04:07.545662Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:04:07.545662Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"OcFkT6lv3CaxrXeBTfgkOkNGkVhdiY3OItD+M4e3656Ai17/pq6XvccV5KclXn7c40Nm7f4xV2528LpgowlbBg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:04:07.546327Z","signed_message":"canonical_sha256_bytes"},"source_id":"1807.00116","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:441e52d971bf732d1d8a69bb943ca3ab0c8969d63bae2f90472f65908abdca3b","sha256:c114d1ec0d666bbfb0bd945ee9d8f0dbcff07855bf94c8cc2223c40106b60dc0"],"state_sha256":"605ce1b97c7ecd6e453e4d3815b29a7af378924bdb9543d520657b0b2a45211b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vehI/RqItxCecAm8dmSSkkMJdZfNYoD5+yZwbmAyVf9Gj/rbfI46zN5BzA/2xEM0ObK1aLdhlx8RmmnkdauvBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-20T08:40:15.121137Z","bundle_sha256":"c40cfe5a21cbfeec264739aece7751dc8027ad0312a223b455fe32e1674b94ac"}}