{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:JZSTBQGY7U54GZJVARFSNGVWY3","short_pith_number":"pith:JZSTBQGY","canonical_record":{"source":{"id":"1705.05716","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-05-16T14:15:27Z","cross_cats_sorted":[],"title_canon_sha256":"6581b15f3e56bfcd277dd43750860430dbd29b689ed87d28b8084b6f4b593350","abstract_canon_sha256":"8e005299ec984f2c0ba593ba1018748bdd60d5b8a6e2dad6b1a195df1af7a134"},"schema_version":"1.0"},"canonical_sha256":"4e6530c0d8fd3bc36535044b269ab6c6e60ae2d93dd6ca46ad8bc8aa24952643","source":{"kind":"arxiv","id":"1705.05716","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.05716","created_at":"2026-05-18T00:37:33Z"},{"alias_kind":"arxiv_version","alias_value":"1705.05716v1","created_at":"2026-05-18T00:37:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.05716","created_at":"2026-05-18T00:37:33Z"},{"alias_kind":"pith_short_12","alias_value":"JZSTBQGY7U54","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_16","alias_value":"JZSTBQGY7U54GZJV","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_8","alias_value":"JZSTBQGY","created_at":"2026-05-18T12:31:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:JZSTBQGY7U54GZJVARFSNGVWY3","target":"record","payload":{"canonical_record":{"source":{"id":"1705.05716","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-05-16T14:15:27Z","cross_cats_sorted":[],"title_canon_sha256":"6581b15f3e56bfcd277dd43750860430dbd29b689ed87d28b8084b6f4b593350","abstract_canon_sha256":"8e005299ec984f2c0ba593ba1018748bdd60d5b8a6e2dad6b1a195df1af7a134"},"schema_version":"1.0"},"canonical_sha256":"4e6530c0d8fd3bc36535044b269ab6c6e60ae2d93dd6ca46ad8bc8aa24952643","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:33.711980Z","signature_b64":"2/ACr9wIU4VsoWE4vtkdgTT24mPplWM4KtHvGnHk+6xtSTALdOEWzFy50xxyqjaPej1Xi2ck7x0GkA/9tLgGAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4e6530c0d8fd3bc36535044b269ab6c6e60ae2d93dd6ca46ad8bc8aa24952643","last_reissued_at":"2026-05-18T00:37:33.711560Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:33.711560Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1705.05716","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":"2026-05-18T00:37:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3KO7wCr/ClxPr1VVcA16xWu30RTI2JqjMZCcJa1+GbkdHRA4oIluKkyXyUDMs1XJCEk02wz+BxtxsEBjWMY1DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T21:36:54.074664Z"},"content_sha256":"05a9b0f066333a3b3a407df0fe6fc56fa3a0d2a9fdff574cd637d7a2e6ac1285","schema_version":"1.0","event_id":"sha256:05a9b0f066333a3b3a407df0fe6fc56fa3a0d2a9fdff574cd637d7a2e6ac1285"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:JZSTBQGY7U54GZJVARFSNGVWY3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nonequilibrium Langevin dynamics: a demonstration study of shear flow fluctuations in a simple fluid","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"E.G.D. Cohen, Lamberto Rondoni, Roman Belousov","submitted_at":"2017-05-16T14:15:27Z","abstract_excerpt":"The present study is based on a recent success of the second-order stochastic fluctuation theory in describing time autocorrelations of equilibrium and nonequilibrium physical systems. In particular, it was shown to yield values of the related deterministic parameters of the Langevin equation for a Couette flow in a microscopic Molecular Dynamics model of a simple fluid. In this paper we find all the remaining constants of the stochastic dynamics, which is then numerically simulated and directly compared with the original physical system. By using these data, we study in detail the accuracy an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.05716","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":"2026-05-18T00:37:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mhdG0nLhCJrbtOPzVVYeV77nZQKAyVCo+Vl5bYSqbG2jG9VPDFtLjB0VkdfqFsBsSaPHINdnn5Odh/fpwrWuBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T21:36:54.075044Z"},"content_sha256":"4c4344461d780a29c92ef43b633a6753a8d7990636815e8d02a45443ede7129c","schema_version":"1.0","event_id":"sha256:4c4344461d780a29c92ef43b633a6753a8d7990636815e8d02a45443ede7129c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JZSTBQGY7U54GZJVARFSNGVWY3/bundle.json","state_url":"https://pith.science/pith/JZSTBQGY7U54GZJVARFSNGVWY3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JZSTBQGY7U54GZJVARFSNGVWY3/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":"2026-05-27T21:36:54Z","links":{"resolver":"https://pith.science/pith/JZSTBQGY7U54GZJVARFSNGVWY3","bundle":"https://pith.science/pith/JZSTBQGY7U54GZJVARFSNGVWY3/bundle.json","state":"https://pith.science/pith/JZSTBQGY7U54GZJVARFSNGVWY3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JZSTBQGY7U54GZJVARFSNGVWY3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:JZSTBQGY7U54GZJVARFSNGVWY3","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":"8e005299ec984f2c0ba593ba1018748bdd60d5b8a6e2dad6b1a195df1af7a134","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-05-16T14:15:27Z","title_canon_sha256":"6581b15f3e56bfcd277dd43750860430dbd29b689ed87d28b8084b6f4b593350"},"schema_version":"1.0","source":{"id":"1705.05716","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.05716","created_at":"2026-05-18T00:37:33Z"},{"alias_kind":"arxiv_version","alias_value":"1705.05716v1","created_at":"2026-05-18T00:37:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.05716","created_at":"2026-05-18T00:37:33Z"},{"alias_kind":"pith_short_12","alias_value":"JZSTBQGY7U54","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_16","alias_value":"JZSTBQGY7U54GZJV","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_8","alias_value":"JZSTBQGY","created_at":"2026-05-18T12:31:24Z"}],"graph_snapshots":[{"event_id":"sha256:4c4344461d780a29c92ef43b633a6753a8d7990636815e8d02a45443ede7129c","target":"graph","created_at":"2026-05-18T00:37:33Z","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":"The present study is based on a recent success of the second-order stochastic fluctuation theory in describing time autocorrelations of equilibrium and nonequilibrium physical systems. In particular, it was shown to yield values of the related deterministic parameters of the Langevin equation for a Couette flow in a microscopic Molecular Dynamics model of a simple fluid. In this paper we find all the remaining constants of the stochastic dynamics, which is then numerically simulated and directly compared with the original physical system. By using these data, we study in detail the accuracy an","authors_text":"E.G.D. Cohen, Lamberto Rondoni, Roman Belousov","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-05-16T14:15:27Z","title":"Nonequilibrium Langevin dynamics: a demonstration study of shear flow fluctuations in a simple fluid"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.05716","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":"sha256:05a9b0f066333a3b3a407df0fe6fc56fa3a0d2a9fdff574cd637d7a2e6ac1285","target":"record","created_at":"2026-05-18T00:37:33Z","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":"8e005299ec984f2c0ba593ba1018748bdd60d5b8a6e2dad6b1a195df1af7a134","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-05-16T14:15:27Z","title_canon_sha256":"6581b15f3e56bfcd277dd43750860430dbd29b689ed87d28b8084b6f4b593350"},"schema_version":"1.0","source":{"id":"1705.05716","kind":"arxiv","version":1}},"canonical_sha256":"4e6530c0d8fd3bc36535044b269ab6c6e60ae2d93dd6ca46ad8bc8aa24952643","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4e6530c0d8fd3bc36535044b269ab6c6e60ae2d93dd6ca46ad8bc8aa24952643","first_computed_at":"2026-05-18T00:37:33.711560Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:37:33.711560Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2/ACr9wIU4VsoWE4vtkdgTT24mPplWM4KtHvGnHk+6xtSTALdOEWzFy50xxyqjaPej1Xi2ck7x0GkA/9tLgGAg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:37:33.711980Z","signed_message":"canonical_sha256_bytes"},"source_id":"1705.05716","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:05a9b0f066333a3b3a407df0fe6fc56fa3a0d2a9fdff574cd637d7a2e6ac1285","sha256:4c4344461d780a29c92ef43b633a6753a8d7990636815e8d02a45443ede7129c"],"state_sha256":"547f0dd24ab601753f47f48bec7964bce16561ab7f965457c2ec11223b42535b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yxfhS2d8Aqd+vvIt1KZ5BmsS2ov2x20a2eB3xYGINqXSQhp9EPSnGZBQqZZ4XC2d5EIi47k6c+st1fk/RAPBCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T21:36:54.078379Z","bundle_sha256":"7549b8b356519227d75aa1f659c028c0f0b0e3ad3396abc0e0ee0b6d22311b74"}}