Definition 28.3.1 (Modular Function).label Let $G$ be a locally compact group and $\mu$ be a left Haar measure on $G$, then

  1. (1)

    For any $f, g \in C_{c}^{+}(G; \real) \setminus \bracs{0}$, $A, B \in \cb_{G}$ with $\mu(A), \mu(B) > 0$, and $y \in G$,

    \[\Delta_{G}(y) = \frac{\int R_{y^{-1}}f d\mu}{\int f d\mu}= \frac{\int R_{y^{-1}}g d\mu}{\int g d\mu}= \frac{\mu(Ay)}{\mu(A)}= \frac{\mu(By)}{\mu(B)}> 0\]

  2. (2)

    For each $y \in G$ and $A \in \cb_{G}$, denote $\mu_{y}(A) = \mu(Ay)$, then $\mu_{y}(dx) = \Delta_{G}(y)\mu(dx)$.

  3. (3)

    For any choice of $f \in C_{c}^{+}(G; \real) \setminus \bracs{0}$, the mapping $\Delta_{G}: G \to (0, \infty)$ defined by $y \mapsto \int R_{y^{-1}}f d\mu$ is a continuous group homomorphism.

  4. (4)

    For each $A \in \cb_{G}$, let $\nu(A) = \mu(A^{-1})$, then $\nu(dx) = \Delta(x^{-1})\mu(dx)$.

The homomorphism $\Delta_{G}: G \to (0, \infty)$ is the modular function of $G$.

Proof, [Proposition 2.24, Proposition 2.31, Fol16]. (1), (2): For each $y \in G$, $\mu_{y}$ is also a left Haar measure. By [Haar’s Theorem]theorem:haar, there exists $\lambda > 0$ such that $\mu_{y} = \lambda \mu$. In which case,

\[\Delta_{G}(y^{-1}) = \frac{\int R_{y} f d\mu}{\int f d\mu}= \frac{\int R_{y} g d\mu}{\int g d\mu}= \frac{\mu(Ay)}{\mu(A)}= \frac{\mu(By)}{\mu(B)}\]

(3): By Proposition 28.2.8, the mapping $y \mapsto \int R_{y} f d\mu$ is continuous. For any $x, y \in G$ and $A \in \cb_{G}$ with $\mu(A) > 0$,

\[\Delta_{G}(xy)\mu(A) = \mu(Axy) = \Delta_{G}(y)\mu(Ax) = \Delta_{G}(y)\Delta_{G}(x)\mu(A)\]

(4): Let $f \in C_{c}^{+}(G)$ and $y \in G$, then

\begin{align*}\int R_{y}f(x) \Delta_{G}(x^{-1})\mu(dx)&= \Delta_{G}(y)\int f(xy)\Delta_{G}[(xy)^{-1}]\mu(dx) \\&= \int f(x)\Delta(x^{-1})\mu(dx)\end{align*}

so $\Delta_{G}(x^{-1})\mu(dx)$ is a right Haar measure. By Haar’s Theorem, there exists $\lambda > 0$ such that $\nu(dx) = \lambda \Delta_{G}(x^{-1})\mu(dx)$.

If $\lambda \ne 1$, then there exists $U \in \cn_{G}(1)$ symmetric and compact such that $|\Delta_{G}(x^{-1}) - 1| \le 2^{-1}|\lambda - 1|$ on $U$. In which case, by symmetry, $\mu(U) = \nu(U)$, and

\begin{align*}|\lambda - 1|\mu(U)&= |\lambda \nu(U) - \mu(U)| = \abs{\int_U \Delta_G(x^{-1})-1 \mu(dx)}\\&\le \frac{1}{2}|\lambda - 1|\mu(U)\end{align*}

which contradicts the fact that $\lambda \ne 1$. Therefore $\lambda = 1$, and $\nu(dx) = \Delta_{G}(x^{-1})\mu(dx)$.$\square$

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