Conformal Group

In mathematics, the conformal group of an inner product space is the group of transformations from the space to itself that preserve angles. More formally, it is the group of transformations that preserve the conformal geometry of the space.

Several specific conformal groups are particularly important:
* The conformal orthogonal group. If ''V'' is a vector space with a quadratic form ''Q'', then the conformal orthogonal group is the group of linear transformations ''T'' of ''V'' for which there exists a scalar ''λ'' such that for all ''x'' in ''V''
*:$Q(Tx) = \lambda^2 Q(x)$
:For a definite quadratic form, the conformal orthogonal group is equal to the orthogonal group times the group of dilations.
* The conformal group of the sphere is generated by the inversions in circles. This group is also known as the Möbius group.
* In Euclidean space E^''n'', , the conformal group is generated by inversions in hyperspheres.
* In a pseudo-Euclidean space E^''p'',''q'', the conformal group is .

All conformal groups are Lie groups.

Angle analysis

In Euclidean geometry one can expect the standard circular angle to be characteristic, but in pseudo-Euclidean space there is also the hyperbolic angle. In the study of special relativity the various frames of reference, for varying velocity with respect to a rest frame, are related by rapidity, a hyperbolic angle. One way to describe a Lorentz boost is as a hyperbolic rotation which preserves the differential angle between rapidities. Thus, they are conformal transformations with respect to the hyperbolic angle.

A method to generate an appropriate conformal group is to mimic the steps of the Möbius group as the conformal group of the ordinary complex plane. Pseudo-Euclidean geometry is supported by alternative complex planes where points are split-complex numbers or dual numbers. Just as the Möbius group requires the Riemann sphere, a compact space, for a complete description, so the alternative complex planes require compactification for complete description of conformal mapping. Nevertheless, the conformal group in each case is given by linear fractional transformations on the appropriate plane.

Mathematical definition

Given a ( Pseudo-)Riemannian manifold $M$ with conformal class /math>, the conformal group $\text(M)$ is the group of conformal maps from $M$ to itself.

More concretely, this is the group of angle-preserving smooth maps from $M$ to itself. However, when the signature of /math> is not definite, the 'angle' is a ''hyper-angle'' which is potentially infinite.

For Pseudo-Euclidean space, the definition is slightly different. $\text(p,q)$ is the conformal group of the manifold arising from conformal compactification of the pseudo-Euclidean space $\mathbf^$ (sometimes identified with $\mathbb^$ after a choice of orthonormal basis). This conformal compactification can be defined using $S^p\times S^q$, considered as a submanifold of null points in $\mathbb^$ by the inclusion $(\mathbf, \mathbf)\mapsto X = (\mathbf, \mathbf)$ (where $X$ is considered as a single spacetime vector). The conformal compactification is then $S^p\times S^q$ with 'antipodal points' identified. This happens by projectivising the space $\mathbb^$. If $N^$ is the conformal compactification, then $\text(p,q) := \text(N^)$. In particular, this group includes inversion of $\mathbb^$, which is not a map from $\mathbb^$ to itself as it maps the origin to infinity, and maps infinity to the origin.

Conformal group of spacetime

In 1908, Harry Bateman and Ebenezer Cunningham, two young researchers at University of Liverpool, broached the idea of a conformal group of spacetime
They argued that the kinematics groups are perforce conformal as they preserve the quadratic form of spacetime and are akin to orthogonal transformations, though with respect to an isotropic quadratic form. The liberties of an electromagnetic field are not confined to kinematic motions, but rather are required only to be locally ''proportional to'' a transformation preserving the quadratic form. Harry Bateman's paper in 1910 studied the Jacobian matrix of a transformation that preserves the light cone and showed it had the conformal property (proportional to a form preserver). Bateman and Cunningham showed that this conformal group is "the largest group of transformations leaving Maxwell’s equations structurally invariant." The conformal group of spacetime has been denoted

Isaak Yaglom has contributed to the mathematics of spacetime conformal transformations in split-complex and dual numbers. Since split-complex numbers and dual numbers form rings, not fields, the linear fractional transformations require a projective line over a ring to be bijective mappings.

It has been traditional since the work of Ludwik Silberstein in 1914 to use the ring of biquaternions to represent the Lorentz group. For the spacetime conformal group, it is sufficient to consider linear fractional transformations on the projective line over that ring. Elements of the spacetime conformal group were called spherical wave transformations by Bateman. The particulars of the spacetime quadratic form study have been absorbed into Lie sphere geometry.

Commenting on the continued interest shown in physical science, A. O. Barut wrote in 1985, "One of the prime reasons for the interest in the conformal group is that it is perhaps the most important of the larger groups containing the Poincaré group." A. O. Barut & H.-D. Doebner (1985) ''Conformal groups and Related Symmetries: Physical Results and Mathematical Background'', Lecture Notes in Physics #261 Springer books, see preface for quotation

See also

* Conformal map
* Conformal symmetry

References

Further reading

*
* .
* Peter Scherk (1960) "Some Concepts of Conformal Geometry", American Mathematical Monthly 67(1): 1−30 {{doi, 10.2307/2308920
* Martin Schottenloher, The conformal group, chapter 2 of A mathematical introduction to conformal field theory, 2008
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page on conformal groups

Conformal geometry