{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:WXRCV6JU6T43XKGPSXQR73WZNN","short_pith_number":"pith:WXRCV6JU","schema_version":"1.0","canonical_sha256":"b5e22af934f4f9bba8cf95e11feed96b4538fb0118c047bf0c54d50898292891","source":{"kind":"arxiv","id":"2409.04273","version":2},"attestation_state":"computed","paper":{"title":"High-field magnetic phase diagrams of the $\\textit{R}$Mn$_6$Sn$_6$ kagome metals","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Nil L, R. J. McQueeney, Thais Victa-Trevisan","submitted_at":"2024-09-06T13:30:23Z","abstract_excerpt":"$\\textit{R}$Mn$_6$Sn$_6$ ($R=$~Y,~Gd$-$Lu) kagome metals are promising materials hosting flat electronic bands and Dirac points that interact with magnetism. The coupling between the two magnetic $R$ and Mn sublattices can drive complex magnetic states with potential consequences for spin and charge transport and other topological properties. Here, we use a detailed magnetic Hamiltonian to calculate and predict the magnetic phase diagrams for $\\textit{R}$Mn$_6$Sn$_6$ kagome metals within the mean-field approximation. These calculations reveal a variety of collinear, non-collinear, and non-copl"},"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":"2409.04273","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-09-06T13:30:23Z","cross_cats_sorted":[],"title_canon_sha256":"a4a250b76d50120815d07b8a280bedacc68808fe68a819f4ddffdbd7b6ce4403","abstract_canon_sha256":"bfb039d3b2571b59c600167929d786935fd72045a5a2a56deeb40f5430b3efd1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:14:05.163354Z","signature_b64":"oJ2/w0Uur0Byz5/q7JrbjTDhJegpXutbYXHiEsKDjbTzNGtAsSlXROMETqSIWxNkGSH+FqfRdQIDQgFexNupBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b5e22af934f4f9bba8cf95e11feed96b4538fb0118c047bf0c54d50898292891","last_reissued_at":"2026-07-05T10:14:05.162876Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:14:05.162876Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"High-field magnetic phase diagrams of the $\\textit{R}$Mn$_6$Sn$_6$ kagome metals","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Nil L, R. J. McQueeney, Thais Victa-Trevisan","submitted_at":"2024-09-06T13:30:23Z","abstract_excerpt":"$\\textit{R}$Mn$_6$Sn$_6$ ($R=$~Y,~Gd$-$Lu) kagome metals are promising materials hosting flat electronic bands and Dirac points that interact with magnetism. The coupling between the two magnetic $R$ and Mn sublattices can drive complex magnetic states with potential consequences for spin and charge transport and other topological properties. Here, we use a detailed magnetic Hamiltonian to calculate and predict the magnetic phase diagrams for $\\textit{R}$Mn$_6$Sn$_6$ kagome metals within the mean-field approximation. These calculations reveal a variety of collinear, non-collinear, and non-copl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.04273","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2409.04273/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":"2409.04273","created_at":"2026-07-05T10:14:05.162932+00:00"},{"alias_kind":"arxiv_version","alias_value":"2409.04273v2","created_at":"2026-07-05T10:14:05.162932+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.04273","created_at":"2026-07-05T10:14:05.162932+00:00"},{"alias_kind":"pith_short_12","alias_value":"WXRCV6JU6T43","created_at":"2026-07-05T10:14:05.162932+00:00"},{"alias_kind":"pith_short_16","alias_value":"WXRCV6JU6T43XKGP","created_at":"2026-07-05T10:14:05.162932+00:00"},{"alias_kind":"pith_short_8","alias_value":"WXRCV6JU","created_at":"2026-07-05T10:14:05.162932+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2504.15926","citing_title":"ErMn$_6$Sn$_6$: A Promising Kagome Antiferromagnetic Candidate for Room-Temperature Nernst Effect-based thermoelectrics","ref_index":40,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WXRCV6JU6T43XKGPSXQR73WZNN","json":"https://pith.science/pith/WXRCV6JU6T43XKGPSXQR73WZNN.json","graph_json":"https://pith.science/api/pith-number/WXRCV6JU6T43XKGPSXQR73WZNN/graph.json","events_json":"https://pith.science/api/pith-number/WXRCV6JU6T43XKGPSXQR73WZNN/events.json","paper":"https://pith.science/paper/WXRCV6JU"},"agent_actions":{"view_html":"https://pith.science/pith/WXRCV6JU6T43XKGPSXQR73WZNN","download_json":"https://pith.science/pith/WXRCV6JU6T43XKGPSXQR73WZNN.json","view_paper":"https://pith.science/paper/WXRCV6JU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2409.04273&json=true","fetch_graph":"https://pith.science/api/pith-number/WXRCV6JU6T43XKGPSXQR73WZNN/graph.json","fetch_events":"https://pith.science/api/pith-number/WXRCV6JU6T43XKGPSXQR73WZNN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WXRCV6JU6T43XKGPSXQR73WZNN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WXRCV6JU6T43XKGPSXQR73WZNN/action/storage_attestation","attest_author":"https://pith.science/pith/WXRCV6JU6T43XKGPSXQR73WZNN/action/author_attestation","sign_citation":"https://pith.science/pith/WXRCV6JU6T43XKGPSXQR73WZNN/action/citation_signature","submit_replication":"https://pith.science/pith/WXRCV6JU6T43XKGPSXQR73WZNN/action/replication_record"}},"created_at":"2026-07-05T10:14:05.162932+00:00","updated_at":"2026-07-05T10:14:05.162932+00:00"}