{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:SCONPGISBV4MMUCBSJ6EUDALAU","short_pith_number":"pith:SCONPGIS","schema_version":"1.0","canonical_sha256":"909cd799120d78c65041927c4a0c0b051fbadd6a873a464b312bcf48681bcc1c","source":{"kind":"arxiv","id":"2504.15563","version":1},"attestation_state":"computed","paper":{"title":"Designing Optimal Distorted-Octahedra Superlattices for Strong Topological Hall Effect","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Chuanrui Huo, Dongke Rong, Er-Jia Guo, Jingdi Lu, Jun Chen, Kuijuan Jin, Lingfei Wang, Qianying Wang, Qiao Jin, Qinghua Zhang, Shiqing Deng, Tianyang Wang, Ting Cui, Yiyan Fan","submitted_at":"2025-04-22T03:32:05Z","abstract_excerpt":"Topologically protected spin states hold great promise for applications in next generation of memory circuits and spintronic devices. These intriguing textures typically emerge in bulk materials or heterostructures with broken inversion symmetry, accompanied by an enhanced Dzyaloshinskii-Moriya interaction (DMI). In this study, we successfully induced the topological Hall effect (THE) in atomically designed (DyScO3)n/(SrRuO3)n (DnSn) superlattices over a significant range of temperatures (10~120K) and thicknesses (16~40nm). Using magnetic force microscopy (MFM), we observed the formation and s"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2504.15563","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-04-22T03:32:05Z","cross_cats_sorted":[],"title_canon_sha256":"b8cd31ad743991d8fbe79aec48366fd1cedfc8163ab6c18afa9d05364a5be78d","abstract_canon_sha256":"f071ca874f8461745cb24d93ccb8da631541c043d05932d7eafc663a2480c7e8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:52:26.662968Z","signature_b64":"BP1+AjSsK9bQibDEPs441qKBa8OtGjN6DahU5OThsf3FbVGiPvo5ikfxvBqxMSUVko7nrv5Ag6amMi58p+SLDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"909cd799120d78c65041927c4a0c0b051fbadd6a873a464b312bcf48681bcc1c","last_reissued_at":"2026-07-05T10:52:26.662516Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:52:26.662516Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Designing Optimal Distorted-Octahedra Superlattices for Strong Topological Hall Effect","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Chuanrui Huo, Dongke Rong, Er-Jia Guo, Jingdi Lu, Jun Chen, Kuijuan Jin, Lingfei Wang, Qianying Wang, Qiao Jin, Qinghua Zhang, Shiqing Deng, Tianyang Wang, Ting Cui, Yiyan Fan","submitted_at":"2025-04-22T03:32:05Z","abstract_excerpt":"Topologically protected spin states hold great promise for applications in next generation of memory circuits and spintronic devices. These intriguing textures typically emerge in bulk materials or heterostructures with broken inversion symmetry, accompanied by an enhanced Dzyaloshinskii-Moriya interaction (DMI). In this study, we successfully induced the topological Hall effect (THE) in atomically designed (DyScO3)n/(SrRuO3)n (DnSn) superlattices over a significant range of temperatures (10~120K) and thicknesses (16~40nm). Using magnetic force microscopy (MFM), we observed the formation and s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.15563","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2504.15563/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2504.15563","created_at":"2026-07-05T10:52:26.662573+00:00"},{"alias_kind":"arxiv_version","alias_value":"2504.15563v1","created_at":"2026-07-05T10:52:26.662573+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.15563","created_at":"2026-07-05T10:52:26.662573+00:00"},{"alias_kind":"pith_short_12","alias_value":"SCONPGISBV4M","created_at":"2026-07-05T10:52:26.662573+00:00"},{"alias_kind":"pith_short_16","alias_value":"SCONPGISBV4MMUCB","created_at":"2026-07-05T10:52:26.662573+00:00"},{"alias_kind":"pith_short_8","alias_value":"SCONPGIS","created_at":"2026-07-05T10:52:26.662573+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SCONPGISBV4MMUCBSJ6EUDALAU","json":"https://pith.science/pith/SCONPGISBV4MMUCBSJ6EUDALAU.json","graph_json":"https://pith.science/api/pith-number/SCONPGISBV4MMUCBSJ6EUDALAU/graph.json","events_json":"https://pith.science/api/pith-number/SCONPGISBV4MMUCBSJ6EUDALAU/events.json","paper":"https://pith.science/paper/SCONPGIS"},"agent_actions":{"view_html":"https://pith.science/pith/SCONPGISBV4MMUCBSJ6EUDALAU","download_json":"https://pith.science/pith/SCONPGISBV4MMUCBSJ6EUDALAU.json","view_paper":"https://pith.science/paper/SCONPGIS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2504.15563&json=true","fetch_graph":"https://pith.science/api/pith-number/SCONPGISBV4MMUCBSJ6EUDALAU/graph.json","fetch_events":"https://pith.science/api/pith-number/SCONPGISBV4MMUCBSJ6EUDALAU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SCONPGISBV4MMUCBSJ6EUDALAU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SCONPGISBV4MMUCBSJ6EUDALAU/action/storage_attestation","attest_author":"https://pith.science/pith/SCONPGISBV4MMUCBSJ6EUDALAU/action/author_attestation","sign_citation":"https://pith.science/pith/SCONPGISBV4MMUCBSJ6EUDALAU/action/citation_signature","submit_replication":"https://pith.science/pith/SCONPGISBV4MMUCBSJ6EUDALAU/action/replication_record"}},"created_at":"2026-07-05T10:52:26.662573+00:00","updated_at":"2026-07-05T10:52:26.662573+00:00"}