CONFORMAL SYMMETRY
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:
:
:
:
:
where are the Lorentz generators, generates translations, generates scaling transformations (also known as dilatations or dilations) and generates the special conformal transformations.
The commutation relations, in addition to those of the Poincaré group, are as follows:
: ,
: ,
:
Additionally, is a scalar and is a covariant vector under the Lorentz transformations.
In two dimensional spacetime, the transformations of the conformal group are the conformal transformations.
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:
★ ''N'' = 4 supersymmetric Yang-Mills.
★ The theory over the worldsheet in string theory.
★ superconformal algebra
★ Coleman-Mandula theorem
★ scale invariance
★ renormalization group
The conformal group has the following representation in spacetime:
:
:
:
:
where are the Lorentz generators, generates translations, generates scaling transformations (also known as dilatations or dilations) and generates the special conformal transformations.
The commutation relations, in addition to those of the Poincaré group, are as follows:
: ,
: ,
:
Additionally, is a scalar and is a covariant vector under the Lorentz transformations.
In two dimensional spacetime, the transformations of the conformal group are the conformal transformations.
| Contents |
| Uses |
| See also |
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:
★ ''N'' = 4 supersymmetric Yang-Mills.
★ The theory over the worldsheet in string theory.
See also
★ superconformal algebra
★ Coleman-Mandula theorem
★ scale invariance
★ renormalization group
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