{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.topic/1","content_sha256":"abe65e2032953aa4e80020b983d4ed2a7fc6b96ba0d0946560f4fef2af1cfa19","created":"2026-10-03T07:17:51Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":[],"salt":"af7b5e642cf7ad1a4b4f288765b5d94ee93336827a52a185cd94b49cefd669a1","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"topic"},"content":{"external_id":"cm.triangular-kagome-spin-liquids","field":"cm","n":"1","review_cite":"Y. Zhou, K. Kanoda, T.-K. Ng, Quantum spin liquid states, Reviews of Modern Physics, 2017","review_link":"https://doi.org/10.1103/RevModPhys.89.025003","review_verified":"true","summary":"On triangular and kagome (corner-sharing triangle) lattices, antiparallel spin alignment cannot satisfy every bond, and quantum fluctuations may prevent any order down to zero temperature. The resulting quantum spin liquids are predicted to host spinons, particles that carry spin but no charge.","title":"Spin liquids on triangular and kagome lattices","topic_ref":null,"why":"These lattices are the main test of whether spin liquids with emergent gauge fields occur in simple models and real materials."},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"677def6cee2b4310dbf7fc819c31e2f8a08fa4d8676c34fd7ceecf8b863d1df4","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"cb747d23a1f48402e81f799ecd2328ad3457d06494e3a2b6868b5f41efb6c154","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"2B2xTAGCYub-BrYUUSLQ9DjggkvSPLFHhwkEJAurmHwvPDJUxFEiy6ykE5YPCMiiwbYTFoU7nDajLzbIeOGLAg"},"schema":"pubphys.envelope/1"},"record_hash":"677def6cee2b4310dbf7fc819c31e2f8a08fa4d8676c34fd7ceecf8b863d1df4","leaf_index":177}