{"schema":"pubphys.bundle/1","record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.revision/1","content_sha256":"2ec19677d4d2b40058ae120f2ffcf33d8cf2d79c3d81f59793f8a9e99c784a17","created":"2026-10-03T07:17:54Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":["5475cf5dc5b1a72283d26dc95dc6e00d7ea4e00096a7c6492e409a1816eeb011"],"salt":"9e9f43d0412bd8a55c083c1b89f552cca45ca3448ed86092499e12059c36c2ac","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"revision"},"content":{"answer_type":"classification","assisted_by":[],"external_id":"amo.rydberg-arrays.kagome-blockade-liquid","kind":"well-posed","literature_status":"contested","n":"1","parents":[],"plain":"Atoms on a kagome lattice (corner-sharing triangles) that block their neighbours from being excited showed, in early calculations, a disordered region that might be a quantum spin liquid. Later calculations found glassy behaviour or no liquid at all.","posed_since":"2021","precise":"H = sum_i (Omega/2) X_i - Delta n_i + sum_i