44.2 Group von Neumann Algebras

Definition 44.2.1 (Group von Neumann Algebra).label Let $G$ be a locally compact group,

\[\lambda: G \to U(L^{2}(G; \complex)) \quad x \mapsto L_{x}\]

be the left regular representation of $G$, and

\[\lambda: L^{1}(G; \complex) \to B(L^{2}(G; \complex)) \quad \lambda(f)(g) = (f * g)\]

be its extension to $L^{1}(G; \complex)$, then

\[L(G) := \lambda(G)'' = \lambda(L^{1}(G;\complex))''\]

is the group von Neumann algebra of $G$. Similarly, if $\rho: G \to U(L^{2}(G; \complex))$ is the right regular representation of $G$, then $R(G) := \rho(G)'' = \rho(L^{1}(G;\complex))''$.

Proof. Firstly, for each $f \in L^{1}(G; \complex)$ and $g, h \in L^{2}(G; \complex)$, by the Fubini-Tonelli Theorem,

\begin{align*}\dpn{\lambda(f)g, h}{L^2(G; \complex)}&= \int_{G} f(x)\dpn{L_xg, h}{L^2(G; \complex)}dx = \iint_{G \times G}f(x) g(x^{-1}y) \ol{h}(y) dy dx \\&= \iint_{G \times G}f(x) g(x^{-1}y)dx \ol{h}(y) dy \\&= \int_{G} (f * g)(y) \ol{h}(y)dy = \dpn{(f * g), h}{L^2(G; \complex)}\end{align*}

By Theorem 32.2.2, $\ol{\lambda(G)}^{\text{\small SOT}}= \ol{\lambda(L^1(G;\complex))}^{\text{\small SOT}}$.$\square$

Definition 44.2.2 (Left Convolver).label Let $G$ be a locally compact group and $f: G \to \complex$ be Borel measurable, then $f$ is a left convolver if for each $g \in L^{2}(G; \complex)$, $\int_{G} |f(y)||g(y^{-1}x)|dy < \infty$ for almost every $x \in G$ and $f * g \in L^{2}(G; \complex)$. The mapping $L_{f}: L^{2}(G; \complex) \to L^{2}(G; \complex)$ defined by $g \mapsto f * g$ is the left convolution map by $f$.

Lemma 44.2.3.label Let $G$ be a locally compact group and $f \in C_{c}(G; \complex)$, $f$ is a left convolver.

Proof. By Young’s Inequality, for each $g \in L^{2}(G; \complex)$, $\norm{f * g}_{L^2(G; \complex)}\le \norm{f}_{L^1(G; \complex)}\norm{g}_{L^2(G; \complex)}$.$\square$

Lemma 44.2.4.label Let $G$ be a locally compact group and $f: G \to \complex$ be a left convolver, then:

  1. (1)

    $L_{f} \in B(L^{2}(G; \complex))$.

  2. (2)

    $f \in L_{\text{loc}}^{1}(G; \complex)$.

  3. (3)

    If $f * g = 0$ for all $g \in L^{2}(G; \complex)$, then $f = 0$ locally almost everywhere.

Proof. (1): Let $\seq{g_n}\subset L^{2}(G; \complex)$, $\seq{f * g_n}\subset L^{2}(G; \complex)$, and $g, h \in L^{2}(G; \complex)$ such that $g_{n} \to g$ and $f * g_{n} \to h$ in $L^{2}(G; \complex)$ as $n \to \infty$. After taking a subsequence, assume without loss of generality that:

  1. (i)

    $f * g_{n} \to h$ almost everywhere.

  2. (ii)

    $\sum_{n \in \natp}\norm{g_n - g}_{L^2(G; \complex)}< \infty$.

In which case, for almost every $x \in G$,

\begin{align*}f * (g_{N} - g)(x)&= \int_{G} f(y)(g_{N} - g)(y^{-1}x)dy \\ |f * (g_{N} - g)(x)|&\le \int_{G}|f(y)|\sum_{n \ge N}|(g_{n} - g)(y^{-1}x)| dy\end{align*}

where $\int_{G}|f(y)|\sum_{n \in \natp}|(g_{n} - g)(y^{-1}x)| dy < \infty$ by (ii). As such, by the Dominated Convergence Theorem, $f * g_{N} \to f * g$ almost everywhere. By (i), $f * g = h$ almost everywhere. Therefore the Closed Graph Theorem implies that $L_{f}$ is continuous.

(2): Let $U \in \cn_{G}(1_{G})$ be relatively compact with $U = U^{-1}$, then $\one_{U} \in L^{2}(G; \complex)$, and $\int_{G} |f(y)|\one_{U}(y^{-1}x)dy < \infty$ for almost every $x \in G$. For each $x_{0} \in G$, by Proposition 31.2.7, there exists $x \in G$ such that $x_{0} \in xU$ and $\int_{G} |f(y)|\one_{U}(y^{-1}x)dy < \infty$. As such, for any $K \subset G$ compact, there exists $F \subset G$ finite such that $\int_{G} |f(y)|\one_{U}(y^{-1}x)dy < \infty$ for each $x \in F$ and $K \subset \bigcup_{x \in F}xU$. In which case,

\[\int_{K} |f(y)|dy \le \sum_{x \in F}\int_{G} |f(y)|\one_{U}(y^{-1}x)dy < \infty\]

(3): By Lemma 44.2.4, $f$ is locally integrable. Let $K \subset G$ be relatively compact. Using Lemma 5.20.2, assume without loss of generality that $K$ is also open.

Let $g \in C_{c}(G; \complex)$ with $\supp{g}\subset K^{-1}$, then there exists $V \in \cn_{G}(1_{G})$ such that $\supp{g}^{-1}V \subset K^{-1}$. In which case, for each $x \in V$,

\[(f * g)(x) = \int_{G} f(y)g(y^{-1}x) dy = \int_{K} f(y)g(y^{-1}x) dy = (\one_{K}f * g)(x)\]

so $f * g$ is continuous on $V$ by Young’s Inequality. In particular, $f * g|_{V}= 0$ almost everywhere implies that $\int_{G} f(y)g(y^{-1}) dy = 0$. As such, $\int_{G} fg = 0$ for all $g \in C_{c}(G; \complex)$ with $\supp{g}\subset K$. By uniqueness from the Riesz Representation Theorem, $f|_{K} = 0$ almost everywhere. Therefore $f = 0$ locally almost everywhere.$\square$

Definition 44.2.5 (Space of Left Convolvers).label Let $G$ be a group, $LC(G) := \bracsn{L_f| f: G \to \complex\text{ is a left convolver}}\subset B(l^{2}(G; \complex))$, and $f, g: G \to \complex$ be left convolvers, then:

  1. (1)

    $f \in l^{2}(G; \complex)$.

  2. (2)

    $L_{f}^{*} = L_{f^*}$, where $f^{*}(x) = \ol{f(x^{-1})}$ for all $x \in G$.

  3. (3)

    $L_{f * g}= L_{f}L_{g}$.

  4. (4)

    $LC(G) \subset B(l^{2}(G; \complex))$ is a von Neumann algebra.

The set $LC(G)$ is the algebra of left convolvers on $G$.

Proof, [Proposition 1.3.5, AP]. (1): $f * \delta_{e} = f \in l^{2}(G; \complex)$.

(2): Let $x, y \in G$, then

\begin{align*}\dpn{L_f\delta_x, \delta_y}{l^2(G; \complex)}&= (f * \delta_{x})(y) = f(yx^{-1}) \\ \dpn{\delta_x, L_{f^*}\delta_y}{l^2(G;\complex)}&= \ol{(f^* * \delta_y)(x)}= \ol{f^*(xy^{-1})}= f(yx^{-1})\end{align*}

(3): By (1), $f * g \in l^{2}(G; \complex)$ is defined. For any $h \in l^{2}(G; \complex)$, by associativity of convolution,

\[L_{f * g}h = (f * g) * h = f * (g * h) = L_{f}L_{g}h\]

(4): Let $T \in \ol{LC(G)}^{\text{\small SOT}}$ and $\angles{f_\alpha}_{\alpha \in A}$ be left convolvers such that $T = \sotlim_{\alpha \in A}L_{f_\alpha}$. Let $f = T\delta_{e} \in l^{2}(G; \complex)$, then

\[f = T\delta_{e} = \paren{\sotlim_{\alpha \in A}L_{f_\alpha}}\delta_{e} = l^{2}\text{-}\lim_{\alpha \in A}f_{\alpha} * \delta_{e}\]

For any $g \in l^{2}(G; \complex)$,

\[\norm{Tg - f * g}_{l^\infty(G; \complex)}\le \limsup_{\alpha \in A}\norm{g}_{l^2(G; \complex)}\norm{f - f_\alpha}_{l^2(G; \complex)}= 0\]

by Young’s Inequality. Therefore $Tg = f * g$, $T = L_{f}$, and $LC(G)$ is strong-operator closed. By von Neumann’s Bicommutant Theorem, $LC(G)$ is a von Neumann algebra.$\square$

Theorem 44.2.6.label Let $G$ be a group, then $L(G) = LC(G) = R(G)'$.

Proof, [Theorem 1.3.6, AP]. ($\subset$): For any $x, y, z \in G$ and $f \in l^{2}(G; \complex)$,

\[(\lambda(x)\rho(y)f)(z) = (\rho(y)f)(x^{-1}z) = f(x^{-1}zy) = (\lambda(x)f)(zy) = (\rho(y)\lambda(x)f)(z)\]

so $\lambda(G) \subset R(G)'$. By Definition 44.2.5, $L(G) \subset LC(G) \subset R(G)'$.

($\supset$): Let $T \in R(G)'$ and $f = T\delta_{e} \in l^{2}(G; \complex)$, then for each $x \in G$,

\[T\delta_{x} = T\rho(x^{-1})\delta_{e} = \rho(x^{-1})T\delta_{e} = f * \delta_{x}\]

As such, $Tg = f * g$ for all $g \in l^{2}(G; \complex)$, and $T = L_{f}$.$\square$

Definition 44.2.7.label Let $G$ be a group. For each $x \in G$, let $u_{x} = \lambda(x)$ and identify it with $\delta_{x}$, then $\lambda(G) = \bracsn{u_x|x \in G}$ are the canonical unitaries of $L(G)$.

For each $f \in l^{2}(G)$, $f = \sum_{x \in G}f(x)u_{x}$. In particular, for each $T \in L(G) = LC(G) \subset l^{2}(G; \complex)$, there exists $\bracsn{T_x}_{x \in G}\subset \complex$ such that $T$ may be written as $T = \sum_{x \in G}T_{x} u_{x}$[1]. In which case, the scalars $\bracsn{T_x}_{x \in G}$ are the Fourier coefficients of $T$.

Definition 44.2.8 (ICC).label Let $G$ be a group, then $G$ has infinite conjugacy classes (ICC) if every non-trivial conjugacy class of $G$ is infinite.

Proposition 44.2.9.label Let $G$ be a group, then the following are equivalent:

  1. (1)

    $L(G)$ is a factor.

  2. (2)

    $G$ is ICC.

Proof, [Proposition 1.3.9, AP]. (2) $\Rightarrow$ (1): Let $T \in Z(L(G))$, then for each $x \in G$,

\[T\delta_{e} = \lambda(x)T\lambda(x^{-1})\delta_{e} = \lambda(x)T\rho(x)\delta_{e} = \lambda(x)\rho(x)(T\delta_{e})\]

so $T\delta_{e}$ is invariant under conjugation, and hence constant on conjugacy classes of $G$.

Since $G$ is ICC and $T\delta_{e} \in l^{2}(G; \complex)$, there exists $\lambda \in \complex$ with $T\delta_{e} = \lambda \delta_{e}$. As such, $T = \lambda I$, and $Z(L(G)) = \complex I$.

$\neg$ (2) $\Rightarrow$ $\neg$ (1): Let $C \subset G$ be a non-trivial finite conjugacy class, then for each $x \in G$, $\delta_{x} * \one_{C} = \one_{xC}= \one_{Cx}= \one_{C} * \delta_{x}$, so $L_{\one_C}$ is a non-trivial element of $Z(L(G))$.$\square$

Definition 44.2.10 (Wreath Product).label Let $H$ be a non-trivial group, $\Gamma$ be a group acting on a set $I$, $H^{(I)}= \bigoplus_{i \in I}H$, and $\Gamma$ act on $H^{(I)}$ by left translation ($(\gamma \xi)_{i} = \xi_{\gamma^{-1}i}$), then the generalised wreath product $H \wr_{I} \Gamma$ is the semidirect product $H^{(I)}\rtimes \Gamma$. The wreath product $H \wr \Gamma$ is the special case where $I = \Gamma$, and $\Gamma$ acts by left translation.

Proposition 44.2.11.label Let $H$ be a non-trivial group, $\Gamma$ be a group acting on a set $I$, and $\Gamma_{f} \subset \Gamma$ be the subgroup of elements whose conjugacy class is finite. If

  1. (a)

    The orbits of $\Gamma \curvearrowleft I$ are infinite.

  2. (b)

    The restricted action $\Gamma_{f} \curvearrowright I$ is faithful.

then the wreath product $H \wr_{I} \Gamma$ is ICC.

Proof, [Proposition 1.3.10, AP]. For each $g \in H \wr_{I} \Gamma$ and subgroup $K \subset H \wr_{I} \Gamma$, let $g^{K} = \bracsn{kgk^{-1}|k \in K}$.

Let $g = (\xi, \gamma) \in H \wr_{I} \Gamma$. First suppose that $\xi \ne e_{H^{(I)}}$, then the support of $\xi$ is non-empty. By (a), the support of $\xi$ has infinite orbit under $\Gamma$, so $g^{G} \supset g^{\Gamma}$ is infinite.

Now suppose that $\xi = e_{H^{(I)}}$ and $\gamma \ne e_{\Gamma}$. If $\gamma \in \Gamma \setminus \Gamma_{f}$, then the conjugacy class of $\gamma$ is infinite, and the conjugacy class of $g$ is also infinite. Now suppose that $\gamma \in \Gamma_{f}$. By (b), there exists $i_{0} \in I$ with $\gamma i_{0} \ne i_{0}$. As $H$ is non-trivial, there exists $\xi_{0} \in H^{(I)}\setminus \bracsn{e_{H^{(I)}}}$ with support $\bracsn{i_0}$. In which case, if $g_{0} = (\xi_{0}, e_{\Gamma})$, then

\[g_{0}^{-1}gg_{0} = (\xi_{0}^{-1}\gamma\xi_{0}, \gamma)\]

and hence $g$ has infinite conjugacy class because $\xi_{0}^{-1}\gamma\xi_{0} \ne e_{H^{(I)}}$. Therefore $g^{G}$ is also infinite.$\square$

  1. This sum does not converge in the strong-operator or the weak-operator topology. keyboard_return

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