{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:GATRPSR3AFWPWND5Z4SBOA6XSZ","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":"2444074aad28933ceec32348d16f465d1f92567fbb4a6fb964da0aaba57aa6c7","cross_cats_sorted":["physics.app-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-12-18T02:15:40Z","title_canon_sha256":"ad19562248c8a419b3802652237463864432da1ec15b2f4554bd3122bf9eb225"},"schema_version":"1.0","source":{"id":"2212.08991","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2212.08991","created_at":"2026-07-05T05:26:16Z"},{"alias_kind":"arxiv_version","alias_value":"2212.08991v1","created_at":"2026-07-05T05:26:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.08991","created_at":"2026-07-05T05:26:16Z"},{"alias_kind":"pith_short_12","alias_value":"GATRPSR3AFWP","created_at":"2026-07-05T05:26:16Z"},{"alias_kind":"pith_short_16","alias_value":"GATRPSR3AFWPWND5","created_at":"2026-07-05T05:26:16Z"},{"alias_kind":"pith_short_8","alias_value":"GATRPSR3","created_at":"2026-07-05T05:26:16Z"}],"graph_snapshots":[{"event_id":"sha256:d75cb316cd612ab1228936a1725470eae92ea3a8555b362234374cfc9b314dc7","target":"graph","created_at":"2026-07-05T05:26:16Z","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/2212.08991/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The interplay between dimensionality and topology manifests in magnetism via both exotic texture morphology and novel dynamics. A free magnetic skyrmion exhibits the skyrmion Hall effect under electric currents. Once it is confined in one-dimensional (1D) channels, the skyrmion Hall effect would be suppressed, and the current-driven skyrmion speed should be boosted by the non-adiabatic spin transfer torque \\b{eta}. Here, we experimentally demonstrate that stripes of a spatially modulated spin helix serve as natural 1D channels to restrict skyrmion. Using FeGe as a benchmark, an interstitial sk","authors_text":"Achim Rosch, Binghui Ge, Dongsheng Song, Gen Yin, Haifeng Du, Jiadong Zang, Jialiang Jiang, Jie-Xiang Yu, Mingliang Tian, Peng Zhang, Sergey S. Pershoguba, Weiwei Wang, Wensen Wei, Xiaolong Fan","cross_cats":["physics.app-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-12-18T02:15:40Z","title":"Experimental observation of one-dimensional motion of interstitial skyrmion in FeGe"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.08991","kind":"arxiv","version":1},"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":"sha256:63cf5dfba46a2e33a7cdc3b300e9ccd4b39d9a4c2742c8608924f4ad8637e234","target":"record","created_at":"2026-07-05T05:26:16Z","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":"2444074aad28933ceec32348d16f465d1f92567fbb4a6fb964da0aaba57aa6c7","cross_cats_sorted":["physics.app-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-12-18T02:15:40Z","title_canon_sha256":"ad19562248c8a419b3802652237463864432da1ec15b2f4554bd3122bf9eb225"},"schema_version":"1.0","source":{"id":"2212.08991","kind":"arxiv","version":1}},"canonical_sha256":"302717ca3b016cfb347dcf241703d79642e74ec212cecc1fdf2160049f3abc18","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"302717ca3b016cfb347dcf241703d79642e74ec212cecc1fdf2160049f3abc18","first_computed_at":"2026-07-05T05:26:16.693306Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:26:16.693306Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"j2uIcN4fjhL9pchvkn0916eMFpCcDYlJvquWurCUr8gU/spWM0Ryb6ySwkD3OrvHRa9j8W/ddeQ+GWBRTpIaDg==","signature_status":"signed_v1","signed_at":"2026-07-05T05:26:16.693727Z","signed_message":"canonical_sha256_bytes"},"source_id":"2212.08991","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:63cf5dfba46a2e33a7cdc3b300e9ccd4b39d9a4c2742c8608924f4ad8637e234","sha256:d75cb316cd612ab1228936a1725470eae92ea3a8555b362234374cfc9b314dc7"],"state_sha256":"5bcb145c2eece1467ab1a78e6cb89fc10efcc622fa5471ba38d13f8bba680cfe"}