{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:X7L6YSTONO5BTMY47HK2POGM45","short_pith_number":"pith:X7L6YSTO","canonical_record":{"source":{"id":"1408.5656","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-08-25T03:33:31Z","cross_cats_sorted":[],"title_canon_sha256":"8152064d545131fc898ff69021050cac7b2a8fa3cf019305e20c3df753806a44","abstract_canon_sha256":"7ba5d7a859e4b498af8f54ac7dc913a3bb479722bc9cf7ae0499b32122e2c984"},"schema_version":"1.0"},"canonical_sha256":"bfd7ec4a6e6bba19b31cf9d5a7b8cce763411d6b411d8fad7399dfca514bd6ef","source":{"kind":"arxiv","id":"1408.5656","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1408.5656","created_at":"2026-05-18T02:44:24Z"},{"alias_kind":"arxiv_version","alias_value":"1408.5656v1","created_at":"2026-05-18T02:44:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.5656","created_at":"2026-05-18T02:44:24Z"},{"alias_kind":"pith_short_12","alias_value":"X7L6YSTONO5B","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"X7L6YSTONO5BTMY4","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"X7L6YSTO","created_at":"2026-05-18T12:28:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:X7L6YSTONO5BTMY47HK2POGM45","target":"record","payload":{"canonical_record":{"source":{"id":"1408.5656","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-08-25T03:33:31Z","cross_cats_sorted":[],"title_canon_sha256":"8152064d545131fc898ff69021050cac7b2a8fa3cf019305e20c3df753806a44","abstract_canon_sha256":"7ba5d7a859e4b498af8f54ac7dc913a3bb479722bc9cf7ae0499b32122e2c984"},"schema_version":"1.0"},"canonical_sha256":"bfd7ec4a6e6bba19b31cf9d5a7b8cce763411d6b411d8fad7399dfca514bd6ef","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:44:24.628125Z","signature_b64":"LTSNKy9db1rdH5UomCwnFzydRIx9C47xm6tXupE/ljbdASmeGHdliPTLS9YJXWKBa/R/MD5LA9A/D+l4cKCUDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bfd7ec4a6e6bba19b31cf9d5a7b8cce763411d6b411d8fad7399dfca514bd6ef","last_reissued_at":"2026-05-18T02:44:24.627748Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:44:24.627748Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1408.5656","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":"2026-05-18T02:44:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"b9DUzAnCLZuCy8zf6k1Oz/1iQuIO7rV8XcIMbVk/tEBn/ImlYcZctK1V/9BmSECC+EIvWc/7+qJiMNbyi+g6Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T10:26:05.659222Z"},"content_sha256":"0152e12722341a490b2d47a53f9ab46383ca3322c0816f343e44d50d1bce89a8","schema_version":"1.0","event_id":"sha256:0152e12722341a490b2d47a53f9ab46383ca3322c0816f343e44d50d1bce89a8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:X7L6YSTONO5BTMY47HK2POGM45","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Corrections to scaling in the dynamic approach to the phase transition with quenched disorder","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"B. Zheng, L. Wang, N. J. Zhou","submitted_at":"2014-08-25T03:33:31Z","abstract_excerpt":"With dynamic Monte Carlo simulations, we investigate the continuous phase transition in the three-dimensional three-state random-bond Potts model. We propose a useful technique to deal with the strong corrections to the dynamic scaling form. The critical point, static exponents $\\beta$ and $\\nu$, and dynamic exponent $z$ are accurately determined. Particularly, the results support that the exponent $\\nu$ satisfies the lower bound $\\nu \\geqslant 2/d$."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.5656","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":"2026-05-18T02:44:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TYIcAbp22TEHsiB8iC4SfvYXrIPjxFqLm6wBw5MxE4tbE05fr/5t304OJBaNJfdgEIJiKm1mOZ+w6sJ8fLTJCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T10:26:05.659578Z"},"content_sha256":"d7d1a966ce2699b33ee039a883c4b1bf4f51cdffc812c2c03f249b4bde8a771d","schema_version":"1.0","event_id":"sha256:d7d1a966ce2699b33ee039a883c4b1bf4f51cdffc812c2c03f249b4bde8a771d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/X7L6YSTONO5BTMY47HK2POGM45/bundle.json","state_url":"https://pith.science/pith/X7L6YSTONO5BTMY47HK2POGM45/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/X7L6YSTONO5BTMY47HK2POGM45/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":"2026-06-04T10:26:05Z","links":{"resolver":"https://pith.science/pith/X7L6YSTONO5BTMY47HK2POGM45","bundle":"https://pith.science/pith/X7L6YSTONO5BTMY47HK2POGM45/bundle.json","state":"https://pith.science/pith/X7L6YSTONO5BTMY47HK2POGM45/state.json","well_known_bundle":"https://pith.science/.well-known/pith/X7L6YSTONO5BTMY47HK2POGM45/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:X7L6YSTONO5BTMY47HK2POGM45","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":"7ba5d7a859e4b498af8f54ac7dc913a3bb479722bc9cf7ae0499b32122e2c984","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-08-25T03:33:31Z","title_canon_sha256":"8152064d545131fc898ff69021050cac7b2a8fa3cf019305e20c3df753806a44"},"schema_version":"1.0","source":{"id":"1408.5656","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1408.5656","created_at":"2026-05-18T02:44:24Z"},{"alias_kind":"arxiv_version","alias_value":"1408.5656v1","created_at":"2026-05-18T02:44:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.5656","created_at":"2026-05-18T02:44:24Z"},{"alias_kind":"pith_short_12","alias_value":"X7L6YSTONO5B","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"X7L6YSTONO5BTMY4","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"X7L6YSTO","created_at":"2026-05-18T12:28:57Z"}],"graph_snapshots":[{"event_id":"sha256:d7d1a966ce2699b33ee039a883c4b1bf4f51cdffc812c2c03f249b4bde8a771d","target":"graph","created_at":"2026-05-18T02:44:24Z","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":"With dynamic Monte Carlo simulations, we investigate the continuous phase transition in the three-dimensional three-state random-bond Potts model. We propose a useful technique to deal with the strong corrections to the dynamic scaling form. The critical point, static exponents $\\beta$ and $\\nu$, and dynamic exponent $z$ are accurately determined. Particularly, the results support that the exponent $\\nu$ satisfies the lower bound $\\nu \\geqslant 2/d$.","authors_text":"B. Zheng, L. Wang, N. J. Zhou","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-08-25T03:33:31Z","title":"Corrections to scaling in the dynamic approach to the phase transition with quenched disorder"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.5656","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":"sha256:0152e12722341a490b2d47a53f9ab46383ca3322c0816f343e44d50d1bce89a8","target":"record","created_at":"2026-05-18T02:44:24Z","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":"7ba5d7a859e4b498af8f54ac7dc913a3bb479722bc9cf7ae0499b32122e2c984","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-08-25T03:33:31Z","title_canon_sha256":"8152064d545131fc898ff69021050cac7b2a8fa3cf019305e20c3df753806a44"},"schema_version":"1.0","source":{"id":"1408.5656","kind":"arxiv","version":1}},"canonical_sha256":"bfd7ec4a6e6bba19b31cf9d5a7b8cce763411d6b411d8fad7399dfca514bd6ef","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bfd7ec4a6e6bba19b31cf9d5a7b8cce763411d6b411d8fad7399dfca514bd6ef","first_computed_at":"2026-05-18T02:44:24.627748Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:44:24.627748Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"LTSNKy9db1rdH5UomCwnFzydRIx9C47xm6tXupE/ljbdASmeGHdliPTLS9YJXWKBa/R/MD5LA9A/D+l4cKCUDg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:44:24.628125Z","signed_message":"canonical_sha256_bytes"},"source_id":"1408.5656","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0152e12722341a490b2d47a53f9ab46383ca3322c0816f343e44d50d1bce89a8","sha256:d7d1a966ce2699b33ee039a883c4b1bf4f51cdffc812c2c03f249b4bde8a771d"],"state_sha256":"bd789c8daa0ee5c258b61e9f871b177c5a396e3f00d4dc7ee0bacbc30d4a2a2e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FQ9nHYRa2LZ+tIIm7ByqDwhO5wr+hDdBUgTFIl2KHemvk78a740+pyczESr08SzL8g2Ejwt4hHvTIGZTTRhpDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T10:26:05.661502Z","bundle_sha256":"dee9289b22d9746ba1a8f39cd3c6d536d0b0a57221e87475f1b7006484ee2540"}}