{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:EKSRVBHN55OTZA65TPCW5MPUMJ","short_pith_number":"pith:EKSRVBHN","schema_version":"1.0","canonical_sha256":"22a51a84edef5d3c83dd9bc56eb1f4626b2e443b5bb3e766ed5db7366e0d9c32","source":{"kind":"arxiv","id":"1006.4235","version":2},"attestation_state":"computed","paper":{"title":"Spin chirality ordering and anomalous Hall effect in the ferromagnetic Kondo lattice model on the triangular lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Yukitoshi Motome, Yutaka Akagi","submitted_at":"2010-06-22T08:56:32Z","abstract_excerpt":"We investigate the ground-state phase diagram for the ferromagnetic Kondo lattice model on a triangular lattice by a variational calculation for various spin orderings up to a four-site unit cell. We find that a noncoplanar four-sublattice ordering with a finite scalar spin chirality emerges at and around 1/4 filling, in addition to the 3/4-filled case, which was predicted to be induced by the perfect nesting of the Fermi surface [I. Martin and C. D. Batista: Phys. Rev. Lett. {\\bf 101} (2008) 156402]. The 1/4-filling phase is stable in a wider range of parameters than the 3/4-filling one, and "},"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":"1006.4235","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2010-06-22T08:56:32Z","cross_cats_sorted":[],"title_canon_sha256":"efc983ceeac96765da8aa6832ab829c7f8655145407a712c555b2ac01371ef28","abstract_canon_sha256":"1a7cb92bb9b6dd1c139e3699152ee6783d57e4f510ab590e1eb2369de529f76c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:42:03.861277Z","signature_b64":"wZ9TWiDkuYDZb1K0zWIWNQtgKejTzlP27tMFF7LHfZWgMUIGMYi1ABSzlPkuHkRszifo5NQKb+xrxbOdKLqkBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"22a51a84edef5d3c83dd9bc56eb1f4626b2e443b5bb3e766ed5db7366e0d9c32","last_reissued_at":"2026-05-18T04:42:03.860742Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:42:03.860742Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Spin chirality ordering and anomalous Hall effect in the ferromagnetic Kondo lattice model on the triangular lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Yukitoshi Motome, Yutaka Akagi","submitted_at":"2010-06-22T08:56:32Z","abstract_excerpt":"We investigate the ground-state phase diagram for the ferromagnetic Kondo lattice model on a triangular lattice by a variational calculation for various spin orderings up to a four-site unit cell. We find that a noncoplanar four-sublattice ordering with a finite scalar spin chirality emerges at and around 1/4 filling, in addition to the 3/4-filled case, which was predicted to be induced by the perfect nesting of the Fermi surface [I. Martin and C. D. Batista: Phys. Rev. Lett. {\\bf 101} (2008) 156402]. The 1/4-filling phase is stable in a wider range of parameters than the 3/4-filling one, and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1006.4235","kind":"arxiv","version":2},"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":"1006.4235","created_at":"2026-05-18T04:42:03.860829+00:00"},{"alias_kind":"arxiv_version","alias_value":"1006.4235v2","created_at":"2026-05-18T04:42:03.860829+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1006.4235","created_at":"2026-05-18T04:42:03.860829+00:00"},{"alias_kind":"pith_short_12","alias_value":"EKSRVBHN55OT","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_16","alias_value":"EKSRVBHN55OTZA65","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_8","alias_value":"EKSRVBHN","created_at":"2026-05-18T12:26:06.534383+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/EKSRVBHN55OTZA65TPCW5MPUMJ","json":"https://pith.science/pith/EKSRVBHN55OTZA65TPCW5MPUMJ.json","graph_json":"https://pith.science/api/pith-number/EKSRVBHN55OTZA65TPCW5MPUMJ/graph.json","events_json":"https://pith.science/api/pith-number/EKSRVBHN55OTZA65TPCW5MPUMJ/events.json","paper":"https://pith.science/paper/EKSRVBHN"},"agent_actions":{"view_html":"https://pith.science/pith/EKSRVBHN55OTZA65TPCW5MPUMJ","download_json":"https://pith.science/pith/EKSRVBHN55OTZA65TPCW5MPUMJ.json","view_paper":"https://pith.science/paper/EKSRVBHN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1006.4235&json=true","fetch_graph":"https://pith.science/api/pith-number/EKSRVBHN55OTZA65TPCW5MPUMJ/graph.json","fetch_events":"https://pith.science/api/pith-number/EKSRVBHN55OTZA65TPCW5MPUMJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EKSRVBHN55OTZA65TPCW5MPUMJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EKSRVBHN55OTZA65TPCW5MPUMJ/action/storage_attestation","attest_author":"https://pith.science/pith/EKSRVBHN55OTZA65TPCW5MPUMJ/action/author_attestation","sign_citation":"https://pith.science/pith/EKSRVBHN55OTZA65TPCW5MPUMJ/action/citation_signature","submit_replication":"https://pith.science/pith/EKSRVBHN55OTZA65TPCW5MPUMJ/action/replication_record"}},"created_at":"2026-05-18T04:42:03.860829+00:00","updated_at":"2026-05-18T04:42:03.860829+00:00"}