Conformal symmetry

From Wikipedia, the free encyclopedia
Jump to navigation Jump to search

In mathematical physics, the conformal symmetry of spacetime is expressed by an extension of the Poincaré group. The extension includes special conformal transformations and dilations. In three spatial plus one time dimensions, conformal symmetry has 15 degrees of freedom: ten for the Poincaré group, four for special conformal transformations, and one for a dilation.

Harry Bateman and Ebenezer Cunningham were the first to study the conformal symmetry of Maxwell's equations. They called a generic expression of conformal symmetry a spherical wave transformation.


The conformal group has the following representation:[1]

where are the Lorentz generators, generates translations, generates scaling transformations (also known as dilatations or dilations) and generates the special conformal transformations.

Commutation relations[edit]

The commutation relations are as follows:[1]

other commutators vanish. Here is the Minkowski metric tensor.

Additionally, is a scalar and is a covariant vector under the Lorentz transformations.

The special conformal transformations are given by[2]

where is a parameter describing the transformation. This special conformal transformation can also be written as , where

which shows that it consists of an inversion, followed by a translation, followed by a second inversion.

A coordinate grid prior to a special conformal transformation
The same grid after a special conformal transformation

In two dimensional spacetime, the transformations of the conformal group are the conformal transformations. There are infinitely many of them.

In more than two dimensions, Euclidean conformal transformations map circles to circles, and hyperspheres to hyperspheres with a straight line considered a degenerate circle and a hyperplane a degenerate hypercircle.

In more than two Lorentzian dimensions, conformal transformations map null rays to null rays and light cones to light cones with a null hyperplane being a degenerate light cone.


Conformal field theory[edit]

The largest possible[why?] global symmetry group of a non-supersymmetric interacting field theory is a direct product of the conformal group with an internal group.[3] Such theories are known as conformal field theories.

Second-order phase transitions[edit]

One particular application is to critical phenomena in systems with local interactions. Fluctuations[clarification needed] 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 present in two-dimensional turbulence at high Reynolds number.

High-energy physics[edit]

Many theories studied in high-energy physics admit the conformal symmetry[why?]. A famous[why?] example is the N=4 supersymmetric Yang-Mills theory. Also, the worldsheet in string theory is described by a two-dimensional conformal field theory coupled to the two-dimensional gravity.

See also[edit]


  1. ^ a b Di Francesco; Mathieu, Sénéchal (1997). Conformal field theory. Graduate texts in contemporary physics. Springer. p. 98. ISBN 978-0-387-94785-3.
  2. ^ Di Francesco; Mathieu, Sénéchal (1997). Conformal field theory. Graduate texts in contemporary physics. Springer. p. 97. ISBN 978-0-387-94785-3.
  3. ^ Juan Maldacena; Alexander Zhiboedov (2013). "Constraining conformal field theories with a higher spin symmetry". Journal of Physics A: Mathematical and Theoretical. 46 (21): 214011. arXiv:1112.1016. Bibcode:2013JPhA...46u4011M. doi:10.1088/1751-8113/46/21/214011.