{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:IIHAR37IDISEL2MAGBROMZ3MCU","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":"b742733d0987b6bab049dabe0340a1f566658024dababd5dfe7d8e14c9125172","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-10-29T15:16:07Z","title_canon_sha256":"d3fe82817aae4f2ff11b3dbcbc757006d3dd42f446f5f3b40ac970ff4313132b"},"schema_version":"1.0","source":{"id":"1010.6244","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.6244","created_at":"2026-05-18T02:04:54Z"},{"alias_kind":"arxiv_version","alias_value":"1010.6244v3","created_at":"2026-05-18T02:04:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.6244","created_at":"2026-05-18T02:04:54Z"},{"alias_kind":"pith_short_12","alias_value":"IIHAR37IDISE","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"IIHAR37IDISEL2MA","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"IIHAR37I","created_at":"2026-05-18T12:26:09Z"}],"graph_snapshots":[{"event_id":"sha256:e927cb4cb4035ac94b1630d8dc04053b4da11e4e4af51a730bb59478f86af5ee","target":"graph","created_at":"2026-05-18T02:04:54Z","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":"It is often assumed that for treating numerical (or experimental) data on continuous transitions the formal analysis derived from the Renormalization Group Theory can only be applied over a narrow temperature range, the \"critical region\"; outside this region correction terms proliferate rendering attempts to apply the formalism hopeless. This pessimistic conclusion follows largely from a choice of scaling variables and scaling expressions which is traditional but which is very inefficient for data covering wide temperature ranges. An alternative \"extended caling\" approach can be made where the","authors_text":"I. A. Campbell, P. H. Lundow","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-10-29T15:16:07Z","title":"An extended scaling analysis of the S=1/2 Ising ferromagnet on the simple cubic lattice"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.6244","kind":"arxiv","version":3},"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":"sha256:001cf380543107f8e18b879b2e36764a2b87026b77f35327c2c1c8630c2e26cf","target":"record","created_at":"2026-05-18T02:04:54Z","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":"b742733d0987b6bab049dabe0340a1f566658024dababd5dfe7d8e14c9125172","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-10-29T15:16:07Z","title_canon_sha256":"d3fe82817aae4f2ff11b3dbcbc757006d3dd42f446f5f3b40ac970ff4313132b"},"schema_version":"1.0","source":{"id":"1010.6244","kind":"arxiv","version":3}},"canonical_sha256":"420e08efe81a2445e9803062e6676c15015369cff0f151de931d6e07451a4a5b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"420e08efe81a2445e9803062e6676c15015369cff0f151de931d6e07451a4a5b","first_computed_at":"2026-05-18T02:04:54.867937Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:04:54.867937Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0xrDTKIr2bIwMewghNpzwL/ivp4NaHopByawDNIpXSmP0UPwWhaCjhghR+5lUT7MNIuogtEhYgJIHF1v3NG0DA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:04:54.868541Z","signed_message":"canonical_sha256_bytes"},"source_id":"1010.6244","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:001cf380543107f8e18b879b2e36764a2b87026b77f35327c2c1c8630c2e26cf","sha256:e927cb4cb4035ac94b1630d8dc04053b4da11e4e4af51a730bb59478f86af5ee"],"state_sha256":"15013f69d43f40b5843aaa7cf9c5bc5f0072a766afe7fb85338e84493e9f3569"}