A quantum field theory invariant under scale transformations, describing universal behavior at critical points.Conformal field theory (CFT) is a quantum field theory that is invariant under conformal transformations — transformations that preserve angles but not necessarily distances. This includes scale transformations (zooming in or out) and translations, rotations, and special conformal transformations. The key feature is that the theory looks the same at all length scales, which makes it the natural framework for describing critical points in statistical mechanics, where systems exhibit scale-invariant fluctuations. In particle physics, CFTs are the building blocks of the AdS/CFT correspondence, a duality between gravity in anti-de Sitter space and a conformal field theory on its boundary, which has become a central tool in quantum gravity research.
The foundations were laid in the late 1960s and 1970s by Polyakov, Migdal, and others, with the modern bootstrap approach revived in 2008 by Rattazzi, Rychkov, Tonni, and Vichi. The classification of two-dimensional CFTs was achieved by Belavin, Polyakov, and Zamolodchikov in 1984.
In a CFT, the correlation functions of operators are highly constrained by the symmetry group. The scale invariance implies that operators have a well-defined scaling dimension, and the theory is characterized by a set of 'central charges' that determine how the theory responds to curvature. The operator product expansion (OPE) allows any product of local operators to be expressed as a sum of other local operators, and the associativity of this expansion leads to the conformal bootstrap equations. Solving these equations, often with numerical methods, yields exact results for critical exponents and other universal quantities without needing a microscopic Lagrangian.
CFTs are used to compute critical exponents in condensed matter systems, such as the Ising model, and to study quantum phase transitions. In high-energy physics, they are essential for the AdS/CFT correspondence, used to model strongly coupled plasmas like the quark-gluon plasma.
In two dimensions, the conformal group is infinite-dimensional, which makes CFTs in 2D exactly solvable in many cases, a luxury not available in higher dimensions.







