{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:3ZKT572EFWX537SHLPRNNF3HZ4","short_pith_number":"pith:3ZKT572E","schema_version":"1.0","canonical_sha256":"de553eff442dafddfe475be2d69767cf2ae0516cee13e07ceb0ada11f9f03ccf","source":{"kind":"arxiv","id":"1110.5554","version":1},"attestation_state":"computed","paper":{"title":"Hall effect of spin-chirality origin in a triangular-lattice helimagnet Fe1.3Sb","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"M. Mochizuki, Y. Kaneko, Y. Shiomi, Y. Tokura","submitted_at":"2011-10-25T16:09:10Z","abstract_excerpt":"We report on a topological Hall effect possibly induced by scalar spin chirality in a quasi-two- dimensional helimagnet Fe$_{1+x}$Sb. In the low-temperature region where the spins on interstitial- Fe (concentration $x=0.3$) intervening the $120^\\circ$ spin-ordered triangular planes tend to freeze, a non-trivial component of Hall resistivity with opposite sign of the conventional anomalous Hall term is observed under magnetic field applied perpendicular to the triangular-lattice plane. The observed unconventional Hall effect is ascribed to the scalar spin chirality arising from the heptamer spi"},"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":"1110.5554","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-10-25T16:09:10Z","cross_cats_sorted":[],"title_canon_sha256":"5b44af36b402f8b3a776a6d97cd6c6ba0a83d8ad824a7ac8572b23b734ec8849","abstract_canon_sha256":"a61a37aaeaf118e61dcdd38cde4cbe4b8297e2f674123f4b5d6381e96527638d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:00:04.017688Z","signature_b64":"GhFbIorc2DybV5wVM5YyNJtkBxulrlzMPKAkyi035fMsabqtqkSLTRSJFqwz+gRVCTJthsv/6CqnR4iJRyCbDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"de553eff442dafddfe475be2d69767cf2ae0516cee13e07ceb0ada11f9f03ccf","last_reissued_at":"2026-05-18T02:00:04.017019Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:00:04.017019Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hall effect of spin-chirality origin in a triangular-lattice helimagnet Fe1.3Sb","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"M. Mochizuki, Y. Kaneko, Y. Shiomi, Y. Tokura","submitted_at":"2011-10-25T16:09:10Z","abstract_excerpt":"We report on a topological Hall effect possibly induced by scalar spin chirality in a quasi-two- dimensional helimagnet Fe$_{1+x}$Sb. In the low-temperature region where the spins on interstitial- Fe (concentration $x=0.3$) intervening the $120^\\circ$ spin-ordered triangular planes tend to freeze, a non-trivial component of Hall resistivity with opposite sign of the conventional anomalous Hall term is observed under magnetic field applied perpendicular to the triangular-lattice plane. The observed unconventional Hall effect is ascribed to the scalar spin chirality arising from the heptamer spi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.5554","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":""},"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":"1110.5554","created_at":"2026-05-18T02:00:04.017110+00:00"},{"alias_kind":"arxiv_version","alias_value":"1110.5554v1","created_at":"2026-05-18T02:00:04.017110+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.5554","created_at":"2026-05-18T02:00:04.017110+00:00"},{"alias_kind":"pith_short_12","alias_value":"3ZKT572EFWX5","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_16","alias_value":"3ZKT572EFWX537SH","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_8","alias_value":"3ZKT572E","created_at":"2026-05-18T12:26:20.644004+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/3ZKT572EFWX537SHLPRNNF3HZ4","json":"https://pith.science/pith/3ZKT572EFWX537SHLPRNNF3HZ4.json","graph_json":"https://pith.science/api/pith-number/3ZKT572EFWX537SHLPRNNF3HZ4/graph.json","events_json":"https://pith.science/api/pith-number/3ZKT572EFWX537SHLPRNNF3HZ4/events.json","paper":"https://pith.science/paper/3ZKT572E"},"agent_actions":{"view_html":"https://pith.science/pith/3ZKT572EFWX537SHLPRNNF3HZ4","download_json":"https://pith.science/pith/3ZKT572EFWX537SHLPRNNF3HZ4.json","view_paper":"https://pith.science/paper/3ZKT572E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1110.5554&json=true","fetch_graph":"https://pith.science/api/pith-number/3ZKT572EFWX537SHLPRNNF3HZ4/graph.json","fetch_events":"https://pith.science/api/pith-number/3ZKT572EFWX537SHLPRNNF3HZ4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3ZKT572EFWX537SHLPRNNF3HZ4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3ZKT572EFWX537SHLPRNNF3HZ4/action/storage_attestation","attest_author":"https://pith.science/pith/3ZKT572EFWX537SHLPRNNF3HZ4/action/author_attestation","sign_citation":"https://pith.science/pith/3ZKT572EFWX537SHLPRNNF3HZ4/action/citation_signature","submit_replication":"https://pith.science/pith/3ZKT572EFWX537SHLPRNNF3HZ4/action/replication_record"}},"created_at":"2026-05-18T02:00:04.017110+00:00","updated_at":"2026-05-18T02:00:04.017110+00:00"}