Definition

Let XX be a and let a GG act continuously on XX. The induced action α:GAut(C0(X))\alpha:G\to\operatorname{Aut}(C_0(X)) is

αs(f)(x)=f(s1x).\alpha_s(f)(x)=f(s^{-1}x).

The full transformation-group CC^*-algebra of (G,X)(G,X) is the C0(X)αGC_0(X)\rtimes_\alpha G. Its reduced version is C0(X)α,rGC_0(X)\rtimes_{\alpha,r}G. Thus the object records both the topology of XX and the dynamics of the action; the acting group and the action are part of the defining data.

Covariant description

A of C0(X)αGC_0(X)\rtimes_\alpha G is determined by a (π,U)(\pi,U): a π\pi of C0(X)C_0(X), a UU of GG, and the covariance equations

Usπ(f)Us=π(αs(f)).U_s\pi(f)U_s^*=\pi(\alpha_s(f)).

The full algebra is universal for these pairs. The reduced algebra instead uses . This distinction is essential when the action is not amenable; there is always a canonical quotient from the full algebra to the reduced one Williams, Chapters 2–3.

Standard examples

If XX is a one-point space with the trivial action, the full and reduced transformation-group algebras are respectively the full and reduced group CC^*-algebras of GG. If GG acts on itself by , then C0(G)rGC_0(G)\rtimes_r G is naturally isomorphic to the on L2(G)L^2(G). More generally, transformation-group algebras are the operator algebras attached to dynamical quotients even when the X/GX/G has poor separation properties.

Conventions and scope

This construction concerns an action on a space. A general need not arise from a commutative coefficient algebra.

References
  1. Dana P. Williams, Crossed Products of C-Algebras*, Mathematical Surveys and Monographs 134, American Mathematical Society, 2007. DOI record. Relevant: Chapters 2–3 on crossed products, covariant representations, and transformation groups.