{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:CQXUSUUBBUK6IR6LVAAMSEQASG","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":"7c469de4b18e2e884fc91f6901e081ac4a72793e67d8e88ebad1ab90ce22779e","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2024-08-12T13:27:01Z","title_canon_sha256":"3d5ca6f942f4003414a138ff3fee81e3b0b32ad55447c0cfcdf8dd7c7f091d46"},"schema_version":"1.0","source":{"id":"2408.06136","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2408.06136","created_at":"2026-07-05T09:58:59Z"},{"alias_kind":"arxiv_version","alias_value":"2408.06136v2","created_at":"2026-07-05T09:58:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.06136","created_at":"2026-07-05T09:58:59Z"},{"alias_kind":"pith_short_12","alias_value":"CQXUSUUBBUK6","created_at":"2026-07-05T09:58:59Z"},{"alias_kind":"pith_short_16","alias_value":"CQXUSUUBBUK6IR6L","created_at":"2026-07-05T09:58:59Z"},{"alias_kind":"pith_short_8","alias_value":"CQXUSUUB","created_at":"2026-07-05T09:58:59Z"}],"graph_snapshots":[{"event_id":"sha256:130b84376658af1926d70c110146c1f862b938f097139aa09f795fb80ef69514","target":"graph","created_at":"2026-07-05T09:58:59Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2408.06136/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present the thermal Stoner-Wohlfarth (tSW) model and apply it in the context of Molecular Dynamics simulations. The model is validated against an ensemble of immobilized, randomly oriented uniaxial particles (solid superparamagnet) and a classical dilute ferrofluid for different combinations of anisotropy strength and magnetic field/moment coupling, at a fixed temperature. We compare analytical and simulation results to quantify the viability of the tSW model in reproducing the equilibrium (with and without dipole-dipole interactions) and dynamic (without dipole-dipole interactions) propert","authors_text":"Andrey A. Kuznetsov, Claas Abert, Deniz Mostarac, Dieter Suess, Pedro A. Sanchez, Santiago Helbig, Sofia S. Kantorovich","cross_cats":["cond-mat.soft"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2024-08-12T13:27:01Z","title":"Thermal Stoner-Wohlfarth Model for Magnetodynamics of Single Domain Nanoparticles: Implementation and Validation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.06136","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:c0201a4d91d68a6b8240ffc06c4852ee61f5f6a9fc176bac1a7126376e3e13a6","target":"record","created_at":"2026-07-05T09:58:59Z","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":"7c469de4b18e2e884fc91f6901e081ac4a72793e67d8e88ebad1ab90ce22779e","cross_cats_sorted":["cond-mat.soft"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2024-08-12T13:27:01Z","title_canon_sha256":"3d5ca6f942f4003414a138ff3fee81e3b0b32ad55447c0cfcdf8dd7c7f091d46"},"schema_version":"1.0","source":{"id":"2408.06136","kind":"arxiv","version":2}},"canonical_sha256":"142f4952810d15e447cba800c9120091b7facd3bd8fa052d6adf73cc4d4285a6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"142f4952810d15e447cba800c9120091b7facd3bd8fa052d6adf73cc4d4285a6","first_computed_at":"2026-07-05T09:58:59.380467Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:58:59.380467Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qPfPt/uxCQyIFgfOGQ0oDytkT5362MYDtw1jWL6ps7Ocf+6cwTFyPBpnx9NpKEzUhiYRLIn6GBW1yt7e5DsTBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T09:58:59.380945Z","signed_message":"canonical_sha256_bytes"},"source_id":"2408.06136","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c0201a4d91d68a6b8240ffc06c4852ee61f5f6a9fc176bac1a7126376e3e13a6","sha256:130b84376658af1926d70c110146c1f862b938f097139aa09f795fb80ef69514"],"state_sha256":"637b33c77c815fbe946ce0f598160a75fb1de50d34efbdd43219b4c590932337"}