{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:LPIR5H73J6TN7SDORLZBBYSSA5","short_pith_number":"pith:LPIR5H73","schema_version":"1.0","canonical_sha256":"5bd11e9ffb4fa6dfc86e8af210e25207601c5392e316b8e3aea114e870490ff3","source":{"kind":"arxiv","id":"1710.00304","version":2},"attestation_state":"computed","paper":{"title":"Slater Insulator in Iridate Perovskites with Strong Spin-Orbit Coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. D. Christianson, A. E. Taylor, D. Haskel, D. Meyers, H. Gotou, J. B. Goodenough, J. Chakhalian, J.-G. Cheng, J.-Q. Yan, J.-S. Zhou, M.A. McGuire, Q. Cui, S. Calder, S. Yunoki, W. Fan, X. Li, Y. Choi, Y. Q. Cai, Y. Uwatoko, Y. Y. Jiao","submitted_at":"2017-10-01T07:02:16Z","abstract_excerpt":"The perovskite SrIrO3 is an exotic narrow-band metal owing to a confluence of the strengths of the spin-orbit coupling (SOC) and the electron-electron correlations. It has been proposed that topological and magnetic insulating phases can be achieved by tuning the SOC, Hubbard interactions, and/or lattice symmetry. Here, we report that the substitution of nonmagnetic, isovalent Sn4+ for Ir4+ in the SrIr1-xSnxO3 perovskites synthesized under high pressure leads to a metal-insulator transition to an antiferromagnetic (AF) phase at TN > 225 K. The continuous change of the cell volume as detected b"},"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":"1710.00304","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-10-01T07:02:16Z","cross_cats_sorted":[],"title_canon_sha256":"21120b26c977ea7a5b4c598800227ed6f312b5f07420f60d102e75c7b7ea5731","abstract_canon_sha256":"8fcf7a41f25e033d8852247d35c00f3e733f1e25724f745155205eb180c18005"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:43.128326Z","signature_b64":"FQOq/NbVJZHQlmIipFrqKqMsdcj+cjLJG+LSyM+2FWiL5GInyyePgPwTLBlzbkYqOwSNoNHBa+QuQEWpP6NTDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5bd11e9ffb4fa6dfc86e8af210e25207601c5392e316b8e3aea114e870490ff3","last_reissued_at":"2026-05-18T00:33:43.127659Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:43.127659Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Slater Insulator in Iridate Perovskites with Strong Spin-Orbit Coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. D. Christianson, A. E. Taylor, D. Haskel, D. Meyers, H. Gotou, J. B. Goodenough, J. Chakhalian, J.-G. Cheng, J.-Q. Yan, J.-S. Zhou, M.A. McGuire, Q. Cui, S. Calder, S. Yunoki, W. Fan, X. Li, Y. Choi, Y. Q. Cai, Y. Uwatoko, Y. Y. Jiao","submitted_at":"2017-10-01T07:02:16Z","abstract_excerpt":"The perovskite SrIrO3 is an exotic narrow-band metal owing to a confluence of the strengths of the spin-orbit coupling (SOC) and the electron-electron correlations. It has been proposed that topological and magnetic insulating phases can be achieved by tuning the SOC, Hubbard interactions, and/or lattice symmetry. Here, we report that the substitution of nonmagnetic, isovalent Sn4+ for Ir4+ in the SrIr1-xSnxO3 perovskites synthesized under high pressure leads to a metal-insulator transition to an antiferromagnetic (AF) phase at TN > 225 K. The continuous change of the cell volume as detected b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.00304","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":"1710.00304","created_at":"2026-05-18T00:33:43.127766+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.00304v2","created_at":"2026-05-18T00:33:43.127766+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.00304","created_at":"2026-05-18T00:33:43.127766+00:00"},{"alias_kind":"pith_short_12","alias_value":"LPIR5H73J6TN","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_16","alias_value":"LPIR5H73J6TN7SDO","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_8","alias_value":"LPIR5H73","created_at":"2026-05-18T12:31:28.150371+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/LPIR5H73J6TN7SDORLZBBYSSA5","json":"https://pith.science/pith/LPIR5H73J6TN7SDORLZBBYSSA5.json","graph_json":"https://pith.science/api/pith-number/LPIR5H73J6TN7SDORLZBBYSSA5/graph.json","events_json":"https://pith.science/api/pith-number/LPIR5H73J6TN7SDORLZBBYSSA5/events.json","paper":"https://pith.science/paper/LPIR5H73"},"agent_actions":{"view_html":"https://pith.science/pith/LPIR5H73J6TN7SDORLZBBYSSA5","download_json":"https://pith.science/pith/LPIR5H73J6TN7SDORLZBBYSSA5.json","view_paper":"https://pith.science/paper/LPIR5H73","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.00304&json=true","fetch_graph":"https://pith.science/api/pith-number/LPIR5H73J6TN7SDORLZBBYSSA5/graph.json","fetch_events":"https://pith.science/api/pith-number/LPIR5H73J6TN7SDORLZBBYSSA5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LPIR5H73J6TN7SDORLZBBYSSA5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LPIR5H73J6TN7SDORLZBBYSSA5/action/storage_attestation","attest_author":"https://pith.science/pith/LPIR5H73J6TN7SDORLZBBYSSA5/action/author_attestation","sign_citation":"https://pith.science/pith/LPIR5H73J6TN7SDORLZBBYSSA5/action/citation_signature","submit_replication":"https://pith.science/pith/LPIR5H73J6TN7SDORLZBBYSSA5/action/replication_record"}},"created_at":"2026-05-18T00:33:43.127766+00:00","updated_at":"2026-05-18T00:33:43.127766+00:00"}