{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:JMHTOWIUCWHQCPRVQALVP4BK27","short_pith_number":"pith:JMHTOWIU","schema_version":"1.0","canonical_sha256":"4b0f375914158f013e35801757f02ad7e75d906a2d1bd24c8c4eaf3cd459a0a8","source":{"kind":"arxiv","id":"1804.08630","version":2},"attestation_state":"computed","paper":{"title":"Tuning the $S = 1/2$ square-lattice antiferromagnet Sr$_2$Cu(Te$_{1-x}$W$_x$)O$_6$ from N\\'eel order to quantum disorder to columnar order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"E. Baggio-Saitovitch, E. Sadrollahi, F. J. Litterst, H. C. Walker, I. Terasaki, K. P. Schmidt, M. Karppinen, O. Mustonen, S. Vasala","submitted_at":"2018-04-23T18:00:02Z","abstract_excerpt":"The spin-1/2 square-lattice Heisenberg model is predicted to have a quantum disordered ground state when magnetic frustration is maximized by competing nearest-neighbor $J_1$ and next-nearest-neighbor $J_2$ interactions ($J_2/J_1 \\approx 0.5$). The double perovskites Sr$_2$CuTeO$_6$ and Sr$_2$CuWO$_6$ are isostructural spin-1/2 square-lattice antiferromagnets with N\\'eel ($J_1$ dominates) and columnar ($J_2$ dominates) magnetic order, respectively. Here we characterize the full isostructural solid solution series Sr$_2$Cu(Te$_{1-x}$W$_x$)O$_6$ ($0 \\leq x \\leq 1$) tunable from N\\'eel order to q"},"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":"1804.08630","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-04-23T18:00:02Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"91f2173dd6e81a5d79a28b1be01b420b6e8c3b648ff8924da339f902ed734968","abstract_canon_sha256":"efec6406b5eea556ae0ef29f9c8978d0cb4d96f656da8d23f717fce03544ea9c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:07:34.616391Z","signature_b64":"wOO47inwISGfvxNApT7PMjhMMXbXUzIhWw3NPJ251id+BpL3I8xwgUXHs6rqD4AXeuTIMjMVdxJh4JAlQDpOBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4b0f375914158f013e35801757f02ad7e75d906a2d1bd24c8c4eaf3cd459a0a8","last_reissued_at":"2026-05-18T00:07:34.615651Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:07:34.615651Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Tuning the $S = 1/2$ square-lattice antiferromagnet Sr$_2$Cu(Te$_{1-x}$W$_x$)O$_6$ from N\\'eel order to quantum disorder to columnar order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"E. Baggio-Saitovitch, E. Sadrollahi, F. J. Litterst, H. C. Walker, I. Terasaki, K. P. Schmidt, M. Karppinen, O. Mustonen, S. Vasala","submitted_at":"2018-04-23T18:00:02Z","abstract_excerpt":"The spin-1/2 square-lattice Heisenberg model is predicted to have a quantum disordered ground state when magnetic frustration is maximized by competing nearest-neighbor $J_1$ and next-nearest-neighbor $J_2$ interactions ($J_2/J_1 \\approx 0.5$). The double perovskites Sr$_2$CuTeO$_6$ and Sr$_2$CuWO$_6$ are isostructural spin-1/2 square-lattice antiferromagnets with N\\'eel ($J_1$ dominates) and columnar ($J_2$ dominates) magnetic order, respectively. Here we characterize the full isostructural solid solution series Sr$_2$Cu(Te$_{1-x}$W$_x$)O$_6$ ($0 \\leq x \\leq 1$) tunable from N\\'eel order to q"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1804.08630","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":"1804.08630","created_at":"2026-05-18T00:07:34.615771+00:00"},{"alias_kind":"arxiv_version","alias_value":"1804.08630v2","created_at":"2026-05-18T00:07:34.615771+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1804.08630","created_at":"2026-05-18T00:07:34.615771+00:00"},{"alias_kind":"pith_short_12","alias_value":"JMHTOWIUCWHQ","created_at":"2026-05-18T12:32:31.084164+00:00"},{"alias_kind":"pith_short_16","alias_value":"JMHTOWIUCWHQCPRV","created_at":"2026-05-18T12:32:31.084164+00:00"},{"alias_kind":"pith_short_8","alias_value":"JMHTOWIU","created_at":"2026-05-18T12:32:31.084164+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/JMHTOWIUCWHQCPRVQALVP4BK27","json":"https://pith.science/pith/JMHTOWIUCWHQCPRVQALVP4BK27.json","graph_json":"https://pith.science/api/pith-number/JMHTOWIUCWHQCPRVQALVP4BK27/graph.json","events_json":"https://pith.science/api/pith-number/JMHTOWIUCWHQCPRVQALVP4BK27/events.json","paper":"https://pith.science/paper/JMHTOWIU"},"agent_actions":{"view_html":"https://pith.science/pith/JMHTOWIUCWHQCPRVQALVP4BK27","download_json":"https://pith.science/pith/JMHTOWIUCWHQCPRVQALVP4BK27.json","view_paper":"https://pith.science/paper/JMHTOWIU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1804.08630&json=true","fetch_graph":"https://pith.science/api/pith-number/JMHTOWIUCWHQCPRVQALVP4BK27/graph.json","fetch_events":"https://pith.science/api/pith-number/JMHTOWIUCWHQCPRVQALVP4BK27/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JMHTOWIUCWHQCPRVQALVP4BK27/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JMHTOWIUCWHQCPRVQALVP4BK27/action/storage_attestation","attest_author":"https://pith.science/pith/JMHTOWIUCWHQCPRVQALVP4BK27/action/author_attestation","sign_citation":"https://pith.science/pith/JMHTOWIUCWHQCPRVQALVP4BK27/action/citation_signature","submit_replication":"https://pith.science/pith/JMHTOWIUCWHQCPRVQALVP4BK27/action/replication_record"}},"created_at":"2026-05-18T00:07:34.615771+00:00","updated_at":"2026-05-18T00:07:34.615771+00:00"}