# Representation function

A continuous function $f$ on a topological space $X$ endowed with a continuous action of a group $G$, whose orbit $\{ {g ^ {*} f } : {g \in G } \}$ in the space of all continuous functions on $X$ generates a finite-dimensional subspace. Representation functions are also called spherical, or almost-invariant, functions. The representation functions with values in the field $k = \mathbf R$ or $\mathbf C$ form a $G$-invariant $k$-subalgebra $F ( X, k) _ {G}$ in the algebra $F ( X, k)$ of all $k$-valued continuous functions on $X$. If $X = G$ is a topological group acting on itself by left shifts, $F ( X, k) _ {G} = F ( G, k) _ {G}$ coincides with the subspace in $F ( G, k)$ generated by the matrix elements of finite-dimensional continuous linear representations of $G$. If $G$ is, moreover, a compact group, then one may restrict to matrix elements of irreducible representations. E.g., if $G = T$ is the rotation group of the plane, then the representation functions on $G$ are the trigonometric polynomials. Another example is furnished by the classical spherical functions on the sphere, which are representation functions for the standard action of the rotation group of the sphere.

If $G$ is a compact topological group, continuously acting on a space $X$ that is a countable union of compacta, then $F ( X, k) _ {G}$ is dense in $F ( X, k)$ in the compact-open topology (cf. Peter–Weyl theorem). Analogous statements hold for representation functions of various degrees of smoothness on a differentiable manifold with a smooth action of a compact Lie group. On the other hand, if $G$ does not allow for non-trivial continuous homomorphisms into a compact group (e.g. $G$ is a connected semi-simple Lie group without compact simple factors), then every representation function on a compact space $X$ with continuous action of $G$ is $G$-invariant .

If a smooth action of a compact Lie group $G$ on a differentiable manifold $X$ has only a finite number of orbit types, then the algebra $F ^ { \infty } ( X, k) _ {G}$ of all representation functions of class $C ^ \infty$ is finitely generated over the subalgebra of all $G$-invariant functions of class $C ^ \infty$ (cf. ). In particular, for a homogeneous space $X$ the algebra $F ( X, \mathbf C ) _ {G} = F ^ { \infty } ( X, \mathbf C ) _ {G}$ is finitely generated and can be identified with the algebra of regular functions on the affine homogeneous algebraic variety over $\mathbf C$ whose set of real points coincides with $X$. The problem of decomposing a $G$-module $F ( X, \mathbf C ) _ {G}$ into a direct sum of simple $G$-modules is important for applications. In case $X$ is the symmetric homogeneous space of a compact group $G$ it was solved by E. Cartan .

A generalization of representation functions are representation sections of a vector $G$-bundle $E$ over a $G$-space $X$, i.e. continuous sections whose $G$-orbits generate a finite-dimensional subspace in the space $\Gamma ( E)$ of all continuous sections, e.g. representation tensor fields on smooth manifolds with a smooth action of a Lie group $G$; they form the $G$-submodule $\Gamma ( E) _ {G} \subset \Gamma ( E)$ (cf. ). If $G$ is a compact group, the submodule $\Gamma ( E) _ {G}$ is dense in $\Gamma ( E)$. In case $X$ is the symmetric homogeneous space of $G$, the decomposition of the $G$-module $\Gamma ( E) _ {G}$ into simple components has been studied (cf. ). If $X$ is the compact homogeneous space of a semi-simple Lie group $G$ without compact factors with a connected stationary subgroup, then

$$\mathop{\rm dim} \Gamma ( E) _ {G} < \infty$$

(cf. ).

How to Cite This Entry:
Representation function. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Representation_function&oldid=52073
This article was adapted from an original article by A.L. Onishchik (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article