Definition

Let GG be a . Its measure algebra M(G)M(G) is the of bounded regular complex Borel measures on GG, equipped with the total-variation norm and convolution determined by

Gf(z)d(μν)(z)=GGf(xy)dμ(x)dν(y)\int_G f(z)\,d(\mu*\nu)(z) =\int_G\int_G f(xy)\,d\mu(x)\,d\nu(y)

for every fC0(G)f\in C_0(G). Equivalently, (μν)(E)(\mu*\nu)(E) is obtained by pushing the forward along group multiplication. With this product, M(G)M(G) is a unital whose identity is the point mass δe\delta_e.

Point masses and the group law

For x,yGx,y\in G, convolution satisfies

δxδy=δxy.\delta_x*\delta_y=\delta_{xy}.

Thus xδxx\mapsto\delta_x embeds the group law into the invertible elements of M(G)M(G). The involution is characterized by δx=δx1\delta_x^*=\delta_{x^{-1}} and, on test functions, by conjugation after inversion. Unlike the density formula for L1(G)L^1(G), this measure-level description requires no chosen Haar measure.

Relation to the group algebra

After fixing a left mm, each fL1(G,m)f\in L^1(G,m) determines the measure fdmf\,dm. This identifies the isometrically with a closed in M(G)M(G). Point masses at nondiscrete points are singular with respect to Haar measure, so M(G)M(G) is generally strictly larger than L1(G)L^1(G) Hewitt and Ross, §19.

Examples and scope

If GG is discrete, every bounded measure is an absolutely summable family and M(G)1(G)M(G)\cong\ell^1(G). For nondiscrete GG, M(G)M(G) simultaneously contains integrable densities and atomic measures. On an it is commutative; on a nonabelian group the point-mass calculation shows immediately that it need not be commutative.

References
  1. E. Hewitt and K. A. Ross, Abstract Harmonic Analysis, Volume I, Springer, 1963. DOI record. Relevant: measure algebras and convolution of measures.
  2. H. Reiter and J. D. Stegeman, Classical Harmonic Analysis and Locally Compact Groups, 2nd ed., Oxford University Press, 2000. Publisher record. Relevant: convolution algebras on locally compact groups.