Definition

Let GG be a with left μ\mu and Δ\Delta, normalized by Gh(xg)dμ(x)=Δ(g)1Gh(x)dμ(x)\int_G h(xg)\,d\mu(x)=\Delta(g)^{-1}\int_G h(x)\,d\mu(x). On the L2(G,μ)L^2(G,\mu), the left and right regular representations are

(λ(g)ξ)(x)=ξ(g1x),(ρ(g)ξ)(x)=Δ(g)1/2ξ(xg).(\lambda(g)\xi)(x)=\xi(g^{-1}x),\qquad (\rho(g)\xi)(x)=\Delta(g)^{1/2}\xi(xg).

Both maps are , and their images commute: λ(g)ρ(h)=ρ(h)λ(g)\lambda(g)\rho(h)=\rho(h)\lambda(g). The modular factor is precisely what makes unitary for a left Haar measure; it equals 11 when GG is unimodular. With the displayed conventions, both gλ(g)g\mapsto\lambda(g) and gρ(g)g\mapsto\rho(g) are group homomorphisms.

Unitarity and continuity

Left invariance of μ\mu gives λ(g)ξ2=ξ2\lVert\lambda(g)\xi\rVert_2=\lVert\xi\rVert_2. Right translation changes the squared L2L^2-norm by Δ(g)1\Delta(g)^{-1}, so the factor Δ(g)1/2\Delta(g)^{1/2} makes ρ(g)\rho(g) unitary. Strong continuity follows first for compactly supported continuous functions and then for all of L2(G)L^2(G) by density, as in Folland, §§2.4 and 3.1.

Relation to convolution

For suitable ff, the λ(f)=Gf(g)λ(g)dμ(g)\lambda(f)=\int_G f(g)\lambda(g)\,d\mu(g) acts by left . Its adjoint is λ(f)\lambda(f^*), where ff^* is the . This is the analytic regular representation used to define .

Conventions and scope
References
  1. Gerald B. Folland, A Course in Abstract Harmonic Analysis, 2nd ed., CRC Press, 2016. DOI record. Relevant: §§2.4 and 3.1 on Haar translation and regular unitary representations.