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arxiv: math/0702103 · v1 · submitted 2007-02-05 · 🧮 math.OA

New topics in ergodic theory

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keywords alphaomegaergodicfracactingbiggdynamicalentangled
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The entangled ergodic theorem concerns the study of the convergence in the strong, or merely weak operator topology, of the multiple Cesaro mean $$\frac{1}{N^{k}}\sum_{n_{1},...,n_{k}=0}^{N-1} U^{n_{\a(1)}}A_{1}U^{n_{\a(2)}}... U^{n_{\a(2k-1)}}A_{2k-1}U^{n_{\a(2k)}} ,$$ where $U$ is a unitary operator acting on the Hilbert space $H$, $\a:\{1,..., m\}\mapsto\{1,..., k\}$ is a partition of the set made of $m$ elements in $k$ parts, and finally $A_{1},...,A_{2k-1}$ are bounded operators acting on $H$. While reviewing recent results about the entangled ergodic theorem, we provide some natural applications to dynamical systems based on compact operators. Namely, let $(\mathfrak A,\alpha)$ be a $C^{*}$--dynamical system, where $\mathfrak A=K(H)$, and $\alpha=ad(U)$ is an automorphism implemented by the unitary $U$. We show that $$\lim_{N\to+\infty}\frac{1}{N}\sum_{n=0}^{N-1}\alpha^{n}=E ,$$ pointwise in the weak topology of $\K(H)$. Here, $E$ is a conditional expectation projecting onto the $C^{*}$--subalgebra $$\bigg(\bigoplus_{z\in\sigma_{\mathop{\rm pp}}(U)} E_{z}B(H)E_{z}\bigg)\bigcap K(H) .$$ If in addition $U$ is weakly mixing with $\Omega\in H$ the unique up to a phase, invariant vector under $U$ and $\omega=<\cdot \Omega,\Omega>$, we have the following recurrence result. If $A\in K(H)$ fulfils $\omega(A)>0$, and $0<m_{1}<m_{2}<...<m_{l}$ are natural numbers kept fixed, then there exists an $N_{0}$ such that $$\frac{1}{N}\sum_{n=0}^{N-1}\omega(A\alpha^{nm_{1}}(A)\alpha^{nm_{2}}(A)... \alpha^{nm_{l}}(A))>0$$ for each $N>N_{0}$.

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