Definition

Let GG be a , let HH be a closed subgroup, and let μ\mu be a on the G/HG/H. Write gμ(E)=μ(g1E)g_*\mu(E)=\mu(g^{-1}E) and rg=d(gμ)/dμr_g=d(g_*\mu)/d\mu. The quasi-regular representation of GG on is

(λG/H(g)ξ)(xH)=rg(xH)1/2ξ(g1xH).(\lambda_{G/H}(g)\xi)(xH) =r_g(xH)^{1/2}\xi(g^{-1}xH).

Quasi-invariance makes the derivative exist, and the Radon–Nikodym factor makes every λG/H(g)\lambda_{G/H}(g) unitary. The cocycle identity for rgr_g gives the representation law.

Invariant-measure case

If G/HG/H has a GG-invariant measure, then rg=1r_g=1 and the formula reduces to translation:

(λG/H(g)ξ)(xH)=ξ(g1xH).(\lambda_{G/H}(g)\xi)(xH)=\xi(g^{-1}xH).

By the , such an invariant measure exists exactly when ΔGH=ΔH\Delta_G|_H=\Delta_H. In particular, it exists when HH is compact.

Relationship to induction

The quasi-regular representation is the from the trivial one-dimensional representation of HH. This interpretation explains why it is central to harmonic analysis on quotients: its and invariant vectors record how GG acts on G/HG/H, while induction connects those data to representations of the subgroup Folland, Chapter 6.

Examples and measure-class independence

For H={e}H=\{e\}, the construction is the left on L2(G)L^2(G). For H=GH=G, it is the trivial representation on a one-dimensional . Replacing μ\mu by an equivalent quasi-invariant measure changes the displayed realization but yields a unitarily equivalent representation through multiplication by the square root of the density.

References
  1. G. B. Folland, A Course in Abstract Harmonic Analysis, 2nd ed., CRC Press, 2016. DOI record. Relevant: homogeneous spaces, quasi-invariant measures, and induced representations.
  2. B. Bekka, P. de la Harpe, and A. Valette, Kazhdan's Property (T), Cambridge University Press, 2008. DOI record. Relevant: quasi-regular representations and invariant vectors.