Conformal symmetry

From Wikipedia, the free encyclopedia

In theoretical physics, conformal symmetry is a symmetry under dilatation (scale invariance) and under the special conformal transformations. Together with the Poincaré group these generate the conformal symmetry group.

The conformal group has the following representation in spacetime:

$M_{\mu\nu}\equiv-i(x_\mu\partial_\nu-x_\nu\partial_\mu)$ , $P_\mu\equiv-i\partial_\mu$

$D\equiv-x_\mu\partial^\mu$ , $K_\mu\equiv-{i\over2}(x^2\partial_\mu-2x_\mu x_\nu\partial^\nu)$

Where $M μν$ are the Lorentz generators, $P μ$ generates translations, $D$ generates dilatation and $K μ$ generates the special conformal transformations.

The commutation relations, in addition to those of the Poincaré group, are as follows:

$[D, D] = 0$ , $[D, K μ] = - K μ$

$[D, P μ] = P μ$ , $[K μ, K ν] = 0$

$[K μ, P ν] = η μν D - i M μν$

Additionally, $D$ is a scalar and $K μ$ is a covariant vector under the Lorentz transformations.

In two dimensional spacetime, the transformations of the conformal group are the conformal transformations.

[edit] Uses

The largest possible symmetry group of a non-supersymmetric interacting field theory is a direct product of the conformal group with an internal group. Such theories are known as conformal field theories.

One particular application is to critical phenomena (phase transitions of the second order) in systems with local interactions. The fluctuations in such systems are conformally invariant at the critical point. That allows for classification of universality classes of phase transitions in terms of conformal field theories. Conformal invariance is also discovered in two-dimensional turbulence at high Reynolds number.

Several spaces and theories in high energy physics admit the conformal symmetry: