{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:EWM3IJ4TLRVEJGH6KSALBXT2VJ","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":"1ad019a4f976d9526e7127025f1e0df62d4bbdd7f0a18cefc27d8d188d291032","cross_cats_sorted":["physics.app-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2019-04-01T14:14:41Z","title_canon_sha256":"9c0fd24274c619afab70b14ef660b14b1f132a8d951847ac809bd30a82556ade"},"schema_version":"1.0","source":{"id":"1904.00870","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1904.00870","created_at":"2026-07-05T00:34:14Z"},{"alias_kind":"arxiv_version","alias_value":"1904.00870v2","created_at":"2026-07-05T00:34:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1904.00870","created_at":"2026-07-05T00:34:14Z"},{"alias_kind":"pith_short_12","alias_value":"EWM3IJ4TLRVE","created_at":"2026-07-05T00:34:14Z"},{"alias_kind":"pith_short_16","alias_value":"EWM3IJ4TLRVEJGH6","created_at":"2026-07-05T00:34:14Z"},{"alias_kind":"pith_short_8","alias_value":"EWM3IJ4T","created_at":"2026-07-05T00:34:14Z"}],"graph_snapshots":[{"event_id":"sha256:42d64145c23b66413d234692b371248f2b1aef54bf513a8e96514f1caceecfe9","target":"graph","created_at":"2026-07-05T00:34:14Z","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/1904.00870/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this work, we study the rotating magnetic field driven domain wall (DW) motion in antiferromagnetic nanowires, using the micromagnetic simulations of the classical Heisenberg spin model. We show that in low frequency region, the rotating field alone could efficiently drive the DW motion even in the absence of Dzyaloshinskii-Moriya interaction (DMI). In this case, the DW rotates synchronously with the magnetic field, and a stable precession torque is available and drives the DW motion with a steady velocity. In large frequency region, the DW only oscillates around its equilibrium position an","authors_text":"D. L. Wen, D. Y. Chen, M. H. Qin, M. Zeng, W. H. Li, X. B. Lu, X. S. Gao, Z. Fan, Z. Y. Chen","cross_cats":["physics.app-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2019-04-01T14:14:41Z","title":"Rotating magnetic field driven antiferromagnetic domain wall motion: Role of Dzyaloshinskii-Moriya interaction"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1904.00870","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":"sha256:183ffd7aab458f3fec0cb7322d16e1982893f163c5b02843e1ee41328be2aee0","target":"record","created_at":"2026-07-05T00:34:14Z","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":"1ad019a4f976d9526e7127025f1e0df62d4bbdd7f0a18cefc27d8d188d291032","cross_cats_sorted":["physics.app-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2019-04-01T14:14:41Z","title_canon_sha256":"9c0fd24274c619afab70b14ef660b14b1f132a8d951847ac809bd30a82556ade"},"schema_version":"1.0","source":{"id":"1904.00870","kind":"arxiv","version":2}},"canonical_sha256":"2599b427935c6a4498fe5480b0de7aaa6ddf733b6916b33174869cf2f5325801","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2599b427935c6a4498fe5480b0de7aaa6ddf733b6916b33174869cf2f5325801","first_computed_at":"2026-07-05T00:34:14.778648Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:34:14.778648Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HJP0du8YkhAcpcQWYu6XGGwSdr/RFlHD1cqs4Myzn7L93+OYemDN9ukeV2Hpa2TOQRfVjxOs3NnfcP1UCZluAw==","signature_status":"signed_v1","signed_at":"2026-07-05T00:34:14.779102Z","signed_message":"canonical_sha256_bytes"},"source_id":"1904.00870","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:183ffd7aab458f3fec0cb7322d16e1982893f163c5b02843e1ee41328be2aee0","sha256:42d64145c23b66413d234692b371248f2b1aef54bf513a8e96514f1caceecfe9"],"state_sha256":"507a41f2851812897478fb6e97185193412cb2066a51f82aa200a9aa991cc01a"}