Statement

Let GG be a , let HH be a closed subgroup, and choose left dgdg and dhdh. There are a positive continuous function ρ:G(0,)\rho:G\to(0,\infty), satisfying

ρ(gh)=ρ(g)ΔH(h)ΔG(h),\rho(gh)=\rho(g)\frac{\Delta_H(h)}{\Delta_G(h)},

and a regular measure dg˙d\dot g on the ]] G/HG/H such that every fCc(G)f\in C_c(G) satisfies

Gf(g)ρ(g)dg=G/HHf(gh)dhdg˙.\int_G f(g)\rho(g)\,dg =\int_{G/H}\int_H f(gh)\,dh\,d\dot g.

This is the Weil integration formula for the stated choices and conventions.

Invariant quotient measures

The quotient G/HG/H admits a nonzero GG-invariant regular measure exactly when

ΔGH=ΔH.\Delta_G|_H=\Delta_H.

Under this condition one may take ρ=1\rho=1, so the formula becomes a literal decomposition of Haar integration into integration along the fibers gHgH and integration over the quotient. The quotient measure is then unique up to a positive scalar; its normalization changes inversely when the Haar measure on HH is rescaled Folland, Chapter 2.

Role of the rho-function

When the modular functions do not agree on HH, no invariant quotient measure exists. The rho-function compensates for this mismatch and produces a on G/HG/H. Different admissible rho-functions give equivalent quotient measures, so constructions based only on the measure class, such as the corresponding unitary quotient representation, do not depend on an accidental choice of density.

Standard cases and conventions

If HH is compact, both ΔH\Delta_H and ΔGH\Delta_G|_H are trivial, hence G/HG/H has an invariant measure. Taking H={e}H=\{e\} recovers integration on GG, while H=GH=G reduces the outer integral to a one-point quotient.

References
  1. G. B. Folland, A Course in Abstract Harmonic Analysis, 2nd ed., CRC Press, 2016. DOI record. Relevant: Chapter 2, rho-functions, quotient measures, and Weil's formula.
  2. E. Hewitt and K. A. Ross, Abstract Harmonic Analysis, Volume I, Springer, 1963. DOI record. Relevant: invariant integration on homogeneous spaces.