{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.topic/1","content_sha256":"38f146c4bcd299c5619bc8f5ea09764ed0a4e5698808dab9baff092ce4fa1580","created":"2026-10-03T07:17:52Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":[],"salt":"2c870ec35f967382a290a6d1d731222eac82cb18fd7b1a6db27f032909c29adf","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"topic"},"content":{"external_id":"qft.cft-rg","field":"qft","n":"1","review_cite":"D. Poland, S. Rychkov, A. Vichi, The Conformal Bootstrap: Theory, Numerical Techniques, and Applications, Rev. Mod. Phys. 91, 015002, 2019","review_link":"https://doi.org/10.1103/RevModPhys.91.015002","review_verified":"true","summary":"At a phase transition, matter looks the same at every magnification, and its physics is a conformal field theory. The bootstrap computes such theories from consistency alone, and some gauge theories become scale invariant at long distances only when they contain enough matter.","title":"Conformal bootstrap, critical points and conformal windows","topic_ref":null,"why":"These theories fix the universal numbers measured at critical points and are the end points of the flows that organize all quantum field theories."},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"59b3cca1f32dc01e525b6517c866b60ced9512aa01bc51694ea2f6fc00c1ca06","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"b5834e47284f887084e02470ba9719343777127f7c3dcf7c43f0277cac5a1561","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"hw7lq7WAs22MgCicIZaNv6Qz-Z2J3_du-3DzQZrTZXeH_gxJrOzTnyifaruQPWQb5IX_Ob-ryz-DeRKJ0gp1Cw"},"schema":"pubphys.envelope/1"},"record_hash":"59b3cca1f32dc01e525b6517c866b60ced9512aa01bc51694ea2f6fc00c1ca06","leaf_index":312}