{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:7XU4SUJOHSJRZVG4TVV6T7WH2M","short_pith_number":"pith:7XU4SUJO","canonical_record":{"source":{"id":"1203.4424","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-20T13:19:37Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"3bf5df82b993bace4365bf6d64131b77710042abb0f6430aae786c579eaae5da","abstract_canon_sha256":"21b5360d8a9b0f25de82ace76a5af2eb92db983bacfa03e77907540fc27336bd"},"schema_version":"1.0"},"canonical_sha256":"fde9c9512e3c931cd4dc9d6be9fec7d30337adad693549fa976aeaafdf43fbcd","source":{"kind":"arxiv","id":"1203.4424","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1203.4424","created_at":"2026-05-18T03:59:39Z"},{"alias_kind":"arxiv_version","alias_value":"1203.4424v1","created_at":"2026-05-18T03:59:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.4424","created_at":"2026-05-18T03:59:39Z"},{"alias_kind":"pith_short_12","alias_value":"7XU4SUJOHSJR","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_16","alias_value":"7XU4SUJOHSJRZVG4","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_8","alias_value":"7XU4SUJO","created_at":"2026-05-18T12:26:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:7XU4SUJOHSJRZVG4TVV6T7WH2M","target":"record","payload":{"canonical_record":{"source":{"id":"1203.4424","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-20T13:19:37Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"3bf5df82b993bace4365bf6d64131b77710042abb0f6430aae786c579eaae5da","abstract_canon_sha256":"21b5360d8a9b0f25de82ace76a5af2eb92db983bacfa03e77907540fc27336bd"},"schema_version":"1.0"},"canonical_sha256":"fde9c9512e3c931cd4dc9d6be9fec7d30337adad693549fa976aeaafdf43fbcd","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:59:39.132031Z","signature_b64":"gRpW69XMT/tlxvqGcC8E4t6xUvbIdEJckUbl207Jyhbzi7BXHTRW2RV3sSiZ6hzhvX8yl/hOEaIftfkzZntLCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fde9c9512e3c931cd4dc9d6be9fec7d30337adad693549fa976aeaafdf43fbcd","last_reissued_at":"2026-05-18T03:59:39.131533Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:59:39.131533Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1203.4424","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":"2026-05-18T03:59:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oUdlF7x1llwfbe5T2phkO+1SLPNU6rRcw29rI1vAZmoJQN2DxbP3KehFJVkq2cd72xd6hrbpmFmzsdt7QvPdBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T08:03:28.101200Z"},"content_sha256":"42eeddb15d1898a5141230c62d8e5581d8aa79953f33634f1a3ed4d40acdc33b","schema_version":"1.0","event_id":"sha256:42eeddb15d1898a5141230c62d8e5581d8aa79953f33634f1a3ed4d40acdc33b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:7XU4SUJOHSJRZVG4TVV6T7WH2M","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Inhomogeneities on all scales at a phase transition altered by disorder","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.stat-mech","authors_text":"Ivan Balog, Katarina Uzelac","submitted_at":"2012-03-20T13:19:37Z","abstract_excerpt":"We have done a finite-size scaling study of a continuous phase transition altered by the quenched bond disorder, investigating systems at quasicritical temperatures of each disorder realization by using the equilibriumlike invaded cluster algorithm. Our results indicate that in order to access the thermal critical exponent $y_\\tau$, it is necessary to average the free energy at quasicritical temperatures of each disorder configuration. Despite the thermal fluctuations on the scale of the system at the transition point, we find that spatial inhomogeneities form in the system and become more pro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.4424","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":"2026-05-18T03:59:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lCp7dvpyNjCmPL/7PASbzhy3fQS3kArLzDZWC+AOClYaSEUTFzdVmFAWSGQ4q67IlIiuV+pJwCvxZFavvIY3CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T08:03:28.101928Z"},"content_sha256":"b52c5a798a0f4c7db64f42d2fba151eee62259c02806bed23db01965b8f4a70f","schema_version":"1.0","event_id":"sha256:b52c5a798a0f4c7db64f42d2fba151eee62259c02806bed23db01965b8f4a70f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7XU4SUJOHSJRZVG4TVV6T7WH2M/bundle.json","state_url":"https://pith.science/pith/7XU4SUJOHSJRZVG4TVV6T7WH2M/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7XU4SUJOHSJRZVG4TVV6T7WH2M/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":"2026-05-22T08:03:28Z","links":{"resolver":"https://pith.science/pith/7XU4SUJOHSJRZVG4TVV6T7WH2M","bundle":"https://pith.science/pith/7XU4SUJOHSJRZVG4TVV6T7WH2M/bundle.json","state":"https://pith.science/pith/7XU4SUJOHSJRZVG4TVV6T7WH2M/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7XU4SUJOHSJRZVG4TVV6T7WH2M/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:7XU4SUJOHSJRZVG4TVV6T7WH2M","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":"21b5360d8a9b0f25de82ace76a5af2eb92db983bacfa03e77907540fc27336bd","cross_cats_sorted":["cond-mat.dis-nn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-20T13:19:37Z","title_canon_sha256":"3bf5df82b993bace4365bf6d64131b77710042abb0f6430aae786c579eaae5da"},"schema_version":"1.0","source":{"id":"1203.4424","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1203.4424","created_at":"2026-05-18T03:59:39Z"},{"alias_kind":"arxiv_version","alias_value":"1203.4424v1","created_at":"2026-05-18T03:59:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.4424","created_at":"2026-05-18T03:59:39Z"},{"alias_kind":"pith_short_12","alias_value":"7XU4SUJOHSJR","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_16","alias_value":"7XU4SUJOHSJRZVG4","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_8","alias_value":"7XU4SUJO","created_at":"2026-05-18T12:26:58Z"}],"graph_snapshots":[{"event_id":"sha256:b52c5a798a0f4c7db64f42d2fba151eee62259c02806bed23db01965b8f4a70f","target":"graph","created_at":"2026-05-18T03:59:39Z","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 done a finite-size scaling study of a continuous phase transition altered by the quenched bond disorder, investigating systems at quasicritical temperatures of each disorder realization by using the equilibriumlike invaded cluster algorithm. Our results indicate that in order to access the thermal critical exponent $y_\\tau$, it is necessary to average the free energy at quasicritical temperatures of each disorder configuration. Despite the thermal fluctuations on the scale of the system at the transition point, we find that spatial inhomogeneities form in the system and become more pro","authors_text":"Ivan Balog, Katarina Uzelac","cross_cats":["cond-mat.dis-nn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-20T13:19:37Z","title":"Inhomogeneities on all scales at a phase transition altered by disorder"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.4424","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":"sha256:42eeddb15d1898a5141230c62d8e5581d8aa79953f33634f1a3ed4d40acdc33b","target":"record","created_at":"2026-05-18T03:59:39Z","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":"21b5360d8a9b0f25de82ace76a5af2eb92db983bacfa03e77907540fc27336bd","cross_cats_sorted":["cond-mat.dis-nn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-20T13:19:37Z","title_canon_sha256":"3bf5df82b993bace4365bf6d64131b77710042abb0f6430aae786c579eaae5da"},"schema_version":"1.0","source":{"id":"1203.4424","kind":"arxiv","version":1}},"canonical_sha256":"fde9c9512e3c931cd4dc9d6be9fec7d30337adad693549fa976aeaafdf43fbcd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fde9c9512e3c931cd4dc9d6be9fec7d30337adad693549fa976aeaafdf43fbcd","first_computed_at":"2026-05-18T03:59:39.131533Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:59:39.131533Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gRpW69XMT/tlxvqGcC8E4t6xUvbIdEJckUbl207Jyhbzi7BXHTRW2RV3sSiZ6hzhvX8yl/hOEaIftfkzZntLCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:59:39.132031Z","signed_message":"canonical_sha256_bytes"},"source_id":"1203.4424","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:42eeddb15d1898a5141230c62d8e5581d8aa79953f33634f1a3ed4d40acdc33b","sha256:b52c5a798a0f4c7db64f42d2fba151eee62259c02806bed23db01965b8f4a70f"],"state_sha256":"d2c949759817946e40c7e86d3284b9b65ecf197623dbb6140bb2976d007194e0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"U1sGJHutDN6foYfHWkb7DphVx4GgVg7G73bTQI6+1N84NHHcWs1K51ctbbnQQLWpe2ZPte6GPNgVES6DSL2NBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-22T08:03:28.105542Z","bundle_sha256":"e206662448e6fe9d24af7720dd4cfb64c7b6f80f0b8a9a0a9db6eeb2fd5db6f5"}}