{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:22YL7KRWCPJNQS2JJCGC5CCLGL","short_pith_number":"pith:22YL7KRW","canonical_record":{"source":{"id":"1407.5332","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-07-20T20:00:11Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech"],"title_canon_sha256":"4d91999bbfa2f3ebbb86b3b19d8c859f6503f6570d5904876e8a9fc2bc3513a1","abstract_canon_sha256":"3d0de0903908b7acd8a6536387928d1d7a581304cd0d0757cfc2e4d3632ba317"},"schema_version":"1.0"},"canonical_sha256":"d6b0bfaa3613d2d84b49488c2e884b32ee4a18c9736803d0f953b010c75979e1","source":{"kind":"arxiv","id":"1407.5332","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.5332","created_at":"2026-05-18T01:42:33Z"},{"alias_kind":"arxiv_version","alias_value":"1407.5332v1","created_at":"2026-05-18T01:42:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.5332","created_at":"2026-05-18T01:42:33Z"},{"alias_kind":"pith_short_12","alias_value":"22YL7KRWCPJN","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"22YL7KRWCPJNQS2J","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"22YL7KRW","created_at":"2026-05-18T12:28:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:22YL7KRWCPJNQS2JJCGC5CCLGL","target":"record","payload":{"canonical_record":{"source":{"id":"1407.5332","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-07-20T20:00:11Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech"],"title_canon_sha256":"4d91999bbfa2f3ebbb86b3b19d8c859f6503f6570d5904876e8a9fc2bc3513a1","abstract_canon_sha256":"3d0de0903908b7acd8a6536387928d1d7a581304cd0d0757cfc2e4d3632ba317"},"schema_version":"1.0"},"canonical_sha256":"d6b0bfaa3613d2d84b49488c2e884b32ee4a18c9736803d0f953b010c75979e1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:42:33.677959Z","signature_b64":"vizm9tzrV/lcpdJ2TSbFJCyrFIas+sHmPSlHXTyTHOBj5+XuX3wijxFloprKbPgxSc56uQA0gR+AQYRnvCc+CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d6b0bfaa3613d2d84b49488c2e884b32ee4a18c9736803d0f953b010c75979e1","last_reissued_at":"2026-05-18T01:42:33.677577Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:42:33.677577Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.5332","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":"2026-05-18T01:42:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KTgEyDZOHtsuY381E7Zuu3wHnKDEOTz9Nsn0VlBubm8NufJn4nrHabAgFDBclPCxvmRmR81Vz5x+rF72JawsCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T05:35:53.164590Z"},"content_sha256":"2e63398ec38107cf03524528570a480194a59e345bac7d235f661f17abb4c4d5","schema_version":"1.0","event_id":"sha256:2e63398ec38107cf03524528570a480194a59e345bac7d235f661f17abb4c4d5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:22YL7KRWCPJNQS2JJCGC5CCLGL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"1/f Noise from the Laws of Thermodynamics for Finite-Size Fluctuations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech"],"primary_cat":"cond-mat.mes-hall","authors_text":"Derek M. Nasir, Ralph V. Chamberlin","submitted_at":"2014-07-20T20:00:11Z","abstract_excerpt":"Computer simulations of the Ising model exhibit white noise if thermal fluctuations are governed by Boltzmann's factor alone; whereas we find that the same model exhibits 1/f noise if Boltzmann's factor is extended to include local alignment entropy to all orders. We show that this nonlinear correction maintains maximum entropy during equilibrium fluctuations. Indeed, as with the usual resolution of Gibbs' paradox that avoids net entropy reduction during reversible processes, the correction yields the statistics of indistinguishable particles. The correction also ensures conservation of energy"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.5332","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":"2026-05-18T01:42:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AAq5wWVjaUldIqgkTHsgn2HNKSdNU4m1+e1DNPTxxj8LFWXH9mcRxOR5IYeuN8SDAV9zLMlSX86QsUjdOC2wAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T05:35:53.164958Z"},"content_sha256":"982ebbecad84b75f684dba941db2b74235672d5b55552b2f6b3daa45c547242c","schema_version":"1.0","event_id":"sha256:982ebbecad84b75f684dba941db2b74235672d5b55552b2f6b3daa45c547242c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/22YL7KRWCPJNQS2JJCGC5CCLGL/bundle.json","state_url":"https://pith.science/pith/22YL7KRWCPJNQS2JJCGC5CCLGL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/22YL7KRWCPJNQS2JJCGC5CCLGL/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":"2026-06-02T05:35:53Z","links":{"resolver":"https://pith.science/pith/22YL7KRWCPJNQS2JJCGC5CCLGL","bundle":"https://pith.science/pith/22YL7KRWCPJNQS2JJCGC5CCLGL/bundle.json","state":"https://pith.science/pith/22YL7KRWCPJNQS2JJCGC5CCLGL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/22YL7KRWCPJNQS2JJCGC5CCLGL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:22YL7KRWCPJNQS2JJCGC5CCLGL","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":"3d0de0903908b7acd8a6536387928d1d7a581304cd0d0757cfc2e4d3632ba317","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-07-20T20:00:11Z","title_canon_sha256":"4d91999bbfa2f3ebbb86b3b19d8c859f6503f6570d5904876e8a9fc2bc3513a1"},"schema_version":"1.0","source":{"id":"1407.5332","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.5332","created_at":"2026-05-18T01:42:33Z"},{"alias_kind":"arxiv_version","alias_value":"1407.5332v1","created_at":"2026-05-18T01:42:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.5332","created_at":"2026-05-18T01:42:33Z"},{"alias_kind":"pith_short_12","alias_value":"22YL7KRWCPJN","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"22YL7KRWCPJNQS2J","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"22YL7KRW","created_at":"2026-05-18T12:28:09Z"}],"graph_snapshots":[{"event_id":"sha256:982ebbecad84b75f684dba941db2b74235672d5b55552b2f6b3daa45c547242c","target":"graph","created_at":"2026-05-18T01:42:33Z","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":"Computer simulations of the Ising model exhibit white noise if thermal fluctuations are governed by Boltzmann's factor alone; whereas we find that the same model exhibits 1/f noise if Boltzmann's factor is extended to include local alignment entropy to all orders. We show that this nonlinear correction maintains maximum entropy during equilibrium fluctuations. Indeed, as with the usual resolution of Gibbs' paradox that avoids net entropy reduction during reversible processes, the correction yields the statistics of indistinguishable particles. The correction also ensures conservation of energy","authors_text":"Derek M. Nasir, Ralph V. Chamberlin","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-07-20T20:00:11Z","title":"1/f Noise from the Laws of Thermodynamics for Finite-Size Fluctuations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.5332","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":"sha256:2e63398ec38107cf03524528570a480194a59e345bac7d235f661f17abb4c4d5","target":"record","created_at":"2026-05-18T01:42:33Z","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":"3d0de0903908b7acd8a6536387928d1d7a581304cd0d0757cfc2e4d3632ba317","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-07-20T20:00:11Z","title_canon_sha256":"4d91999bbfa2f3ebbb86b3b19d8c859f6503f6570d5904876e8a9fc2bc3513a1"},"schema_version":"1.0","source":{"id":"1407.5332","kind":"arxiv","version":1}},"canonical_sha256":"d6b0bfaa3613d2d84b49488c2e884b32ee4a18c9736803d0f953b010c75979e1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d6b0bfaa3613d2d84b49488c2e884b32ee4a18c9736803d0f953b010c75979e1","first_computed_at":"2026-05-18T01:42:33.677577Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:42:33.677577Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vizm9tzrV/lcpdJ2TSbFJCyrFIas+sHmPSlHXTyTHOBj5+XuX3wijxFloprKbPgxSc56uQA0gR+AQYRnvCc+CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:42:33.677959Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.5332","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2e63398ec38107cf03524528570a480194a59e345bac7d235f661f17abb4c4d5","sha256:982ebbecad84b75f684dba941db2b74235672d5b55552b2f6b3daa45c547242c"],"state_sha256":"921b4ab36c3484fea4712e0cfce504cad9fab6a2c5421e29d1332b2f914b29ab"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"g5YDAbjEl2jTcsEegCJAqp8ISRvDg/+ZcLW1QqEgSgETx9hZNYY/ddQRK1vSgCaGUsWW8q5lMw7uTuesxhTQDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T05:35:53.167209Z","bundle_sha256":"cea77b9b2115713948ad2f22724a3b77a209602fff5b31563c2c0f506d5cce16"}}