{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:M2BTQ4Q5TCSJZR2BEE3CHGSYJE","short_pith_number":"pith:M2BTQ4Q5","schema_version":"1.0","canonical_sha256":"668338721d98a49cc7412136239a584937a55ae5df3fafc2679826ac1c625351","source":{"kind":"arxiv","id":"2312.01553","version":1},"attestation_state":"computed","paper":{"title":"Emergent electric field induced by current-driven domain wall motion in a room-temperature antiferromagnet FeSn2","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Jun'ichi Ieda, Tomoyuki Yokouchi, Yasufumi Araki, Yuki Shiomi, Yuta Yamane","submitted_at":"2023-12-04T00:50:03Z","abstract_excerpt":"Antiferromagnets have attracted extensive interest as platforms for nanoscale spintronic devices owing to ultrafast spin dynamics and lack of a stray field. One of the crucial missing pieces in antiferromagnets is a quantum-mechanical electric field known as an emergent electric field, which has been observed for the motion of ferromagnetic spin texture. Since this phenomenon allows for the development of novel spintronic devices such as quantum inductors, its identification in antiferromagnets is vital for developing nanoscale spintronic devices. Here, we demonstrate that the motion of antife"},"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":"2312.01553","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2023-12-04T00:50:03Z","cross_cats_sorted":[],"title_canon_sha256":"f2556cb59f438cf49300030d7123ee80e8021cd154a2d54f8b5a7667470e9362","abstract_canon_sha256":"ff653d93304ca848cc8f5733007352b2c791114ff80f9c03306d28d184fbadcd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:19:56.527406Z","signature_b64":"3Upp9z9i2eLWBUE9z4mOrXOIPxV5nnJ2FKiOawbEyiGbqqUqPiGAmeE5L4bgisLNBOXQ4xBF1cEhD+8ksbMxBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"668338721d98a49cc7412136239a584937a55ae5df3fafc2679826ac1c625351","last_reissued_at":"2026-07-05T07:19:56.526937Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:19:56.526937Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Emergent electric field induced by current-driven domain wall motion in a room-temperature antiferromagnet FeSn2","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Jun'ichi Ieda, Tomoyuki Yokouchi, Yasufumi Araki, Yuki Shiomi, Yuta Yamane","submitted_at":"2023-12-04T00:50:03Z","abstract_excerpt":"Antiferromagnets have attracted extensive interest as platforms for nanoscale spintronic devices owing to ultrafast spin dynamics and lack of a stray field. One of the crucial missing pieces in antiferromagnets is a quantum-mechanical electric field known as an emergent electric field, which has been observed for the motion of ferromagnetic spin texture. Since this phenomenon allows for the development of novel spintronic devices such as quantum inductors, its identification in antiferromagnets is vital for developing nanoscale spintronic devices. Here, we demonstrate that the motion of antife"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.01553","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/2312.01553/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":"2312.01553","created_at":"2026-07-05T07:19:56.527012+00:00"},{"alias_kind":"arxiv_version","alias_value":"2312.01553v1","created_at":"2026-07-05T07:19:56.527012+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.01553","created_at":"2026-07-05T07:19:56.527012+00:00"},{"alias_kind":"pith_short_12","alias_value":"M2BTQ4Q5TCSJ","created_at":"2026-07-05T07:19:56.527012+00:00"},{"alias_kind":"pith_short_16","alias_value":"M2BTQ4Q5TCSJZR2B","created_at":"2026-07-05T07:19:56.527012+00:00"},{"alias_kind":"pith_short_8","alias_value":"M2BTQ4Q5","created_at":"2026-07-05T07:19:56.527012+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.16778","citing_title":"Emergent impedance due to antiferromagnetic domain wall dynamics","ref_index":44,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/M2BTQ4Q5TCSJZR2BEE3CHGSYJE","json":"https://pith.science/pith/M2BTQ4Q5TCSJZR2BEE3CHGSYJE.json","graph_json":"https://pith.science/api/pith-number/M2BTQ4Q5TCSJZR2BEE3CHGSYJE/graph.json","events_json":"https://pith.science/api/pith-number/M2BTQ4Q5TCSJZR2BEE3CHGSYJE/events.json","paper":"https://pith.science/paper/M2BTQ4Q5"},"agent_actions":{"view_html":"https://pith.science/pith/M2BTQ4Q5TCSJZR2BEE3CHGSYJE","download_json":"https://pith.science/pith/M2BTQ4Q5TCSJZR2BEE3CHGSYJE.json","view_paper":"https://pith.science/paper/M2BTQ4Q5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2312.01553&json=true","fetch_graph":"https://pith.science/api/pith-number/M2BTQ4Q5TCSJZR2BEE3CHGSYJE/graph.json","fetch_events":"https://pith.science/api/pith-number/M2BTQ4Q5TCSJZR2BEE3CHGSYJE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M2BTQ4Q5TCSJZR2BEE3CHGSYJE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M2BTQ4Q5TCSJZR2BEE3CHGSYJE/action/storage_attestation","attest_author":"https://pith.science/pith/M2BTQ4Q5TCSJZR2BEE3CHGSYJE/action/author_attestation","sign_citation":"https://pith.science/pith/M2BTQ4Q5TCSJZR2BEE3CHGSYJE/action/citation_signature","submit_replication":"https://pith.science/pith/M2BTQ4Q5TCSJZR2BEE3CHGSYJE/action/replication_record"}},"created_at":"2026-07-05T07:19:56.527012+00:00","updated_at":"2026-07-05T07:19:56.527012+00:00"}