{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:2BJO2YCMDYL76CR5IOWYP3RHJT","short_pith_number":"pith:2BJO2YCM","canonical_record":{"source":{"id":"1308.6061","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2013-08-28T05:13:41Z","cross_cats_sorted":["physics.class-ph"],"title_canon_sha256":"4e04f64f34ce2695d83dfe91815586904c72f6df401f971cb82fde2cda0f803a","abstract_canon_sha256":"4d12c0ba5d989992a621d8602085a2bcfb9a75eb58a6b19301b0c635e13b66da"},"schema_version":"1.0"},"canonical_sha256":"d052ed604c1e17ff0a3d43ad87ee274cc115e60a4a13ca73ed3756a09f5e2a63","source":{"kind":"arxiv","id":"1308.6061","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1308.6061","created_at":"2026-05-18T03:07:22Z"},{"alias_kind":"arxiv_version","alias_value":"1308.6061v2","created_at":"2026-05-18T03:07:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.6061","created_at":"2026-05-18T03:07:22Z"},{"alias_kind":"pith_short_12","alias_value":"2BJO2YCMDYL7","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"2BJO2YCMDYL76CR5","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"2BJO2YCM","created_at":"2026-05-18T12:27:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:2BJO2YCMDYL76CR5IOWYP3RHJT","target":"record","payload":{"canonical_record":{"source":{"id":"1308.6061","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2013-08-28T05:13:41Z","cross_cats_sorted":["physics.class-ph"],"title_canon_sha256":"4e04f64f34ce2695d83dfe91815586904c72f6df401f971cb82fde2cda0f803a","abstract_canon_sha256":"4d12c0ba5d989992a621d8602085a2bcfb9a75eb58a6b19301b0c635e13b66da"},"schema_version":"1.0"},"canonical_sha256":"d052ed604c1e17ff0a3d43ad87ee274cc115e60a4a13ca73ed3756a09f5e2a63","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:07:22.776955Z","signature_b64":"GAlyBJ90YMSa8k/pH3CtH48EJNx9X2EqoTJ09Lif2SKnkqZ+KyiteaeWYwj0WeOLNozdDhkxCBZdFMlVGwozDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d052ed604c1e17ff0a3d43ad87ee274cc115e60a4a13ca73ed3756a09f5e2a63","last_reissued_at":"2026-05-18T03:07:22.776368Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:07:22.776368Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1308.6061","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:07:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"v6ExzAvmXgkRzFmTUML5Wy7CUudzuo5Kb++bhE2oAdFsVHBMis45CrLkIu5lOlEX7qdfVwN05hCT2Ff0cuybCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T06:54:45.506923Z"},"content_sha256":"375b51b457132778528f8d30235dd1aeff2d1a8d670e781784c5bd910c17c340","schema_version":"1.0","event_id":"sha256:375b51b457132778528f8d30235dd1aeff2d1a8d670e781784c5bd910c17c340"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:2BJO2YCMDYL76CR5IOWYP3RHJT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Validity of Fourier's law in one-dimensional momentum-conserving lattices with asymmetric interparticle interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.class-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Bambi Hu, Baowen Li, Lei Wang","submitted_at":"2013-08-28T05:13:41Z","abstract_excerpt":"We have numerically studied heat conduction in a few one-dimensional momentum-conserving lattices with asymmetric interparticle interactions by the nonequilibrium heat bath method, the equilibrium Green-Kubo method, and the heat current power spectra analysis. Very strong finite-size effects are clearly observed. Such effects make the heat conduction obey a Fourier-like law in a wide range of lattice lengths. However, in yet longer lattice lengths, the heat conductivity regains its power-law divergence. Therefore the power-law divergence of the heat conductivity in the thermodynamic limit is v"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.6061","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:07:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"65sfDnT5UWXFFbjMPgiWU7VCpkxCk4QP/D74oJomO1AXpwUF7QAaJrZJdRKl0nDlA2BU0SDEYLRVd7v5vLz6Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T06:54:45.507595Z"},"content_sha256":"79354ffe81bd660d72537ba26d095a0fc7797384c4e24619416fee8a9dc7898c","schema_version":"1.0","event_id":"sha256:79354ffe81bd660d72537ba26d095a0fc7797384c4e24619416fee8a9dc7898c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2BJO2YCMDYL76CR5IOWYP3RHJT/bundle.json","state_url":"https://pith.science/pith/2BJO2YCMDYL76CR5IOWYP3RHJT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2BJO2YCMDYL76CR5IOWYP3RHJT/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":"2026-05-31T06:54:45Z","links":{"resolver":"https://pith.science/pith/2BJO2YCMDYL76CR5IOWYP3RHJT","bundle":"https://pith.science/pith/2BJO2YCMDYL76CR5IOWYP3RHJT/bundle.json","state":"https://pith.science/pith/2BJO2YCMDYL76CR5IOWYP3RHJT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2BJO2YCMDYL76CR5IOWYP3RHJT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:2BJO2YCMDYL76CR5IOWYP3RHJT","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":"4d12c0ba5d989992a621d8602085a2bcfb9a75eb58a6b19301b0c635e13b66da","cross_cats_sorted":["physics.class-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2013-08-28T05:13:41Z","title_canon_sha256":"4e04f64f34ce2695d83dfe91815586904c72f6df401f971cb82fde2cda0f803a"},"schema_version":"1.0","source":{"id":"1308.6061","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1308.6061","created_at":"2026-05-18T03:07:22Z"},{"alias_kind":"arxiv_version","alias_value":"1308.6061v2","created_at":"2026-05-18T03:07:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.6061","created_at":"2026-05-18T03:07:22Z"},{"alias_kind":"pith_short_12","alias_value":"2BJO2YCMDYL7","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"2BJO2YCMDYL76CR5","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"2BJO2YCM","created_at":"2026-05-18T12:27:30Z"}],"graph_snapshots":[{"event_id":"sha256:79354ffe81bd660d72537ba26d095a0fc7797384c4e24619416fee8a9dc7898c","target":"graph","created_at":"2026-05-18T03:07:22Z","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":"We have numerically studied heat conduction in a few one-dimensional momentum-conserving lattices with asymmetric interparticle interactions by the nonequilibrium heat bath method, the equilibrium Green-Kubo method, and the heat current power spectra analysis. Very strong finite-size effects are clearly observed. Such effects make the heat conduction obey a Fourier-like law in a wide range of lattice lengths. However, in yet longer lattice lengths, the heat conductivity regains its power-law divergence. Therefore the power-law divergence of the heat conductivity in the thermodynamic limit is v","authors_text":"Bambi Hu, Baowen Li, Lei Wang","cross_cats":["physics.class-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2013-08-28T05:13:41Z","title":"Validity of Fourier's law in one-dimensional momentum-conserving lattices with asymmetric interparticle interactions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.6061","kind":"arxiv","version":2},"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":"sha256:375b51b457132778528f8d30235dd1aeff2d1a8d670e781784c5bd910c17c340","target":"record","created_at":"2026-05-18T03:07:22Z","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":"4d12c0ba5d989992a621d8602085a2bcfb9a75eb58a6b19301b0c635e13b66da","cross_cats_sorted":["physics.class-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2013-08-28T05:13:41Z","title_canon_sha256":"4e04f64f34ce2695d83dfe91815586904c72f6df401f971cb82fde2cda0f803a"},"schema_version":"1.0","source":{"id":"1308.6061","kind":"arxiv","version":2}},"canonical_sha256":"d052ed604c1e17ff0a3d43ad87ee274cc115e60a4a13ca73ed3756a09f5e2a63","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d052ed604c1e17ff0a3d43ad87ee274cc115e60a4a13ca73ed3756a09f5e2a63","first_computed_at":"2026-05-18T03:07:22.776368Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:07:22.776368Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GAlyBJ90YMSa8k/pH3CtH48EJNx9X2EqoTJ09Lif2SKnkqZ+KyiteaeWYwj0WeOLNozdDhkxCBZdFMlVGwozDw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:07:22.776955Z","signed_message":"canonical_sha256_bytes"},"source_id":"1308.6061","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:375b51b457132778528f8d30235dd1aeff2d1a8d670e781784c5bd910c17c340","sha256:79354ffe81bd660d72537ba26d095a0fc7797384c4e24619416fee8a9dc7898c"],"state_sha256":"fc1ec78087a8a06a05c04e31bbfd920920991828913739d78a9498d6a5126950"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KabqzjXDipll0KBEiJhBLSPlb/NFJyyQ86ylmvjreIVjlOpWSFOTzlYfV84kCm6JX7s6/GzydoPTRjaaZ9F1AQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T06:54:45.511714Z","bundle_sha256":"cc9af35886efe52fde006bd2270ae5deb622a70a4a6188b97d32415e60f1b8d2"}}