{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:ENIWHFMVGTHSTMLQHNEASQKQHE","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":"02337999308dfb12993f52935a7216de66a0e4e7c03305d3a4a1805f6785a191","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2017-11-07T04:58:39Z","title_canon_sha256":"aca1c54cea842879d6093c164c7bf474d52958b14e3043c46d59c7843a5ad56d"},"schema_version":"1.0","source":{"id":"1711.02284","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.02284","created_at":"2026-05-18T00:19:25Z"},{"alias_kind":"arxiv_version","alias_value":"1711.02284v2","created_at":"2026-05-18T00:19:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.02284","created_at":"2026-05-18T00:19:25Z"},{"alias_kind":"pith_short_12","alias_value":"ENIWHFMVGTHS","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_16","alias_value":"ENIWHFMVGTHSTMLQ","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_8","alias_value":"ENIWHFMV","created_at":"2026-05-18T12:31:12Z"}],"graph_snapshots":[{"event_id":"sha256:d58dd3e79d0390d9fb3973465663ab88b978672bf40b14041205223641db0bc0","target":"graph","created_at":"2026-05-18T00:19:25Z","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 developed a new algorithm for the stochastic cutoff method, which is a Monte Carlo method for long-range interacting systems. The present new algorithm is efficient for complicated lattice structures, e.g., amorphous and also materials with complicated unit cell structure. In addition, it has an advantage in a high temperature region. With the present method, we investigated an atomistic model of the permanent magnet Nd 2 Fe 14 B with dipole-dipole interactions to study the effect of the anisotropy of the Fe ions on the magnetization structure in the thin film system. It has revealed that t","authors_text":"Masamichi Nishino, Seiji Miyashita, Taichi Hinokihara, Yuta Toga","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2017-11-07T04:58:39Z","title":"Study on Effects of Dipole-dipole Interactions in Nd_2Fe_{14}B thin film Based on Stochastic Cut-off Method with New Efficient Algorithm"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.02284","kind":"arxiv","version":2},"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:dba750931b9881123c2d4a5c3218034894cddb78b829425c0c4a8f9877d8d283","target":"record","created_at":"2026-05-18T00:19:25Z","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":"02337999308dfb12993f52935a7216de66a0e4e7c03305d3a4a1805f6785a191","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2017-11-07T04:58:39Z","title_canon_sha256":"aca1c54cea842879d6093c164c7bf474d52958b14e3043c46d59c7843a5ad56d"},"schema_version":"1.0","source":{"id":"1711.02284","kind":"arxiv","version":2}},"canonical_sha256":"235163959534cf29b1703b48094150392696addd7b31101613fe761cabd14a9f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"235163959534cf29b1703b48094150392696addd7b31101613fe761cabd14a9f","first_computed_at":"2026-05-18T00:19:25.566745Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:19:25.566745Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"lawr88df9A2yOlKfs36v69YT4mXG5HzCKtLvm9YLJoalwszR8qhPx7N9HgpnVseGS385HYT+1Jcgss+eFpssDg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:19:25.567202Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.02284","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:dba750931b9881123c2d4a5c3218034894cddb78b829425c0c4a8f9877d8d283","sha256:d58dd3e79d0390d9fb3973465663ab88b978672bf40b14041205223641db0bc0"],"state_sha256":"f565eba548e588f8f908faf757488dc96dfec3b77c40346dde8a30be86ea4c7c"}