{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:IVRJ76H3KOUEGRQ6MXSDYRCRPD","short_pith_number":"pith:IVRJ76H3","canonical_record":{"source":{"id":"1004.4486","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-04-26T11:27:14Z","cross_cats_sorted":[],"title_canon_sha256":"3b17d8a93831e0e9a36a276786bba16e5c0d0a8b679c188788602b181d44eb35","abstract_canon_sha256":"07b40de8237970da67b003e76f8891523e1b0cd3302489852cbb749bc11c0f38"},"schema_version":"1.0"},"canonical_sha256":"45629ff8fb53a843461e65e43c445178dace90961de2875862ccd5a71c6cc041","source":{"kind":"arxiv","id":"1004.4486","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.4486","created_at":"2026-05-18T03:23:48Z"},{"alias_kind":"arxiv_version","alias_value":"1004.4486v3","created_at":"2026-05-18T03:23:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.4486","created_at":"2026-05-18T03:23:48Z"},{"alias_kind":"pith_short_12","alias_value":"IVRJ76H3KOUE","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"IVRJ76H3KOUEGRQ6","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"IVRJ76H3","created_at":"2026-05-18T12:26:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:IVRJ76H3KOUEGRQ6MXSDYRCRPD","target":"record","payload":{"canonical_record":{"source":{"id":"1004.4486","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-04-26T11:27:14Z","cross_cats_sorted":[],"title_canon_sha256":"3b17d8a93831e0e9a36a276786bba16e5c0d0a8b679c188788602b181d44eb35","abstract_canon_sha256":"07b40de8237970da67b003e76f8891523e1b0cd3302489852cbb749bc11c0f38"},"schema_version":"1.0"},"canonical_sha256":"45629ff8fb53a843461e65e43c445178dace90961de2875862ccd5a71c6cc041","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:48.771689Z","signature_b64":"QHpQIa5c7kiHfmSABg9Q1SYNqRXS3m4Rj4B3IlzvTlgCSgYGjYsH/pBcXfociXR6FyRqDPK7lYGU2ujOACvqCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"45629ff8fb53a843461e65e43c445178dace90961de2875862ccd5a71c6cc041","last_reissued_at":"2026-05-18T03:23:48.771278Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:48.771278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1004.4486","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:23:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"L7Rag2SdVLjJ4yBzhuUBj6CNmISQmu0cfcMz3Mfujp7WJiHSw7izjsj6+vSDSuiEygLKhYbawL9pHJ6/9iixBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T18:21:12.924921Z"},"content_sha256":"e59423407605768050eb321dd32c485415925ea45048d69d95dd5e7fa5b6d624","schema_version":"1.0","event_id":"sha256:e59423407605768050eb321dd32c485415925ea45048d69d95dd5e7fa5b6d624"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:IVRJ76H3KOUEGRQ6MXSDYRCRPD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A Finite Size Scaling Study of Lattice Models in the three-dimensional Ising Universality Class","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Martin Hasenbusch","submitted_at":"2010-04-26T11:27:14Z","abstract_excerpt":"We simulate the spin-1/2 Ising model and the Blume-Capel model at various values of the parameter D on the simple cubic lattice. We perform a finite size scaling study of lattices of a linear size up to L=360 to obtain accurate estimates for critical exponents. We focus on values of D, where the amplitudes of leading corrections are small. Furthermore we employ improved observables that have a small amplitude of the leading correction. We obtain nu=0.63002(10), eta=0.03627(10) and omega=0.832(6). We compare our results with those obtained from previous Monte Carlo simulations and high temperat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.4486","kind":"arxiv","version":3},"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":"2026-05-18T03:23:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZMqaJhrRfz29EB0TQnSvY/rj21KSQxgNpKvz/ovvTxHoS71rONxAK2hOTH6NeemKVgnnr/vwtQBxC0ph5KIwAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T18:21:12.925567Z"},"content_sha256":"162504479ba7505cbf0a2f93712aa9a3bafa06aec1adb6eebb58d8593f5c4340","schema_version":"1.0","event_id":"sha256:162504479ba7505cbf0a2f93712aa9a3bafa06aec1adb6eebb58d8593f5c4340"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IVRJ76H3KOUEGRQ6MXSDYRCRPD/bundle.json","state_url":"https://pith.science/pith/IVRJ76H3KOUEGRQ6MXSDYRCRPD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IVRJ76H3KOUEGRQ6MXSDYRCRPD/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":"2026-08-03T18:21:12Z","links":{"resolver":"https://pith.science/pith/IVRJ76H3KOUEGRQ6MXSDYRCRPD","bundle":"https://pith.science/pith/IVRJ76H3KOUEGRQ6MXSDYRCRPD/bundle.json","state":"https://pith.science/pith/IVRJ76H3KOUEGRQ6MXSDYRCRPD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IVRJ76H3KOUEGRQ6MXSDYRCRPD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:IVRJ76H3KOUEGRQ6MXSDYRCRPD","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":"07b40de8237970da67b003e76f8891523e1b0cd3302489852cbb749bc11c0f38","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-04-26T11:27:14Z","title_canon_sha256":"3b17d8a93831e0e9a36a276786bba16e5c0d0a8b679c188788602b181d44eb35"},"schema_version":"1.0","source":{"id":"1004.4486","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.4486","created_at":"2026-05-18T03:23:48Z"},{"alias_kind":"arxiv_version","alias_value":"1004.4486v3","created_at":"2026-05-18T03:23:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.4486","created_at":"2026-05-18T03:23:48Z"},{"alias_kind":"pith_short_12","alias_value":"IVRJ76H3KOUE","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"IVRJ76H3KOUEGRQ6","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"IVRJ76H3","created_at":"2026-05-18T12:26:09Z"}],"graph_snapshots":[{"event_id":"sha256:162504479ba7505cbf0a2f93712aa9a3bafa06aec1adb6eebb58d8593f5c4340","target":"graph","created_at":"2026-05-18T03:23:48Z","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 simulate the spin-1/2 Ising model and the Blume-Capel model at various values of the parameter D on the simple cubic lattice. We perform a finite size scaling study of lattices of a linear size up to L=360 to obtain accurate estimates for critical exponents. We focus on values of D, where the amplitudes of leading corrections are small. Furthermore we employ improved observables that have a small amplitude of the leading correction. We obtain nu=0.63002(10), eta=0.03627(10) and omega=0.832(6). We compare our results with those obtained from previous Monte Carlo simulations and high temperat","authors_text":"Martin Hasenbusch","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-04-26T11:27:14Z","title":"A Finite Size Scaling Study of Lattice Models in the three-dimensional Ising Universality Class"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.4486","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:e59423407605768050eb321dd32c485415925ea45048d69d95dd5e7fa5b6d624","target":"record","created_at":"2026-05-18T03:23:48Z","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":"07b40de8237970da67b003e76f8891523e1b0cd3302489852cbb749bc11c0f38","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-04-26T11:27:14Z","title_canon_sha256":"3b17d8a93831e0e9a36a276786bba16e5c0d0a8b679c188788602b181d44eb35"},"schema_version":"1.0","source":{"id":"1004.4486","kind":"arxiv","version":3}},"canonical_sha256":"45629ff8fb53a843461e65e43c445178dace90961de2875862ccd5a71c6cc041","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"45629ff8fb53a843461e65e43c445178dace90961de2875862ccd5a71c6cc041","first_computed_at":"2026-05-18T03:23:48.771278Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:23:48.771278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QHpQIa5c7kiHfmSABg9Q1SYNqRXS3m4Rj4B3IlzvTlgCSgYGjYsH/pBcXfociXR6FyRqDPK7lYGU2ujOACvqCA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:23:48.771689Z","signed_message":"canonical_sha256_bytes"},"source_id":"1004.4486","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e59423407605768050eb321dd32c485415925ea45048d69d95dd5e7fa5b6d624","sha256:162504479ba7505cbf0a2f93712aa9a3bafa06aec1adb6eebb58d8593f5c4340"],"state_sha256":"0bc1199cd016906a79747a1052b0f6adb860c593c95e4cb2385078b6f3cd9a19"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mcM7DkpS8Cf1kddsT/eNPlxDmwlvJa7G5cRQWHbI2CkgR/wkepYcgCJrGC8kyCIEDP1Y7H9nqi+FFTXF0ZuGDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T18:21:12.929328Z","bundle_sha256":"eca63ec3f9e34c94a3756f515adfb682348f35437ad9e13b96b76e0260c7f5e0"}}