Weak Hardy Spaces $WH_L^p({\mathbb R}^n)$ Associated to Operators Satisfying $k$-Davies-Gaffney Estimates

Let $L$ be a one-to-one operator of type $ω$ having a bounded $H_\infty$ functional calculus and satisfying the $k$-Davies-Gaffney estimates with $k\in{\mathbb N}$. In this paper, the authors introduce the weak Hardy space $WH_L^p(\mathbb{R}^n)$ associated to $L$ for $p\in (0,\,1]$ via the non-tangential square function $S_L$ and establish a weak molecular characterization of $WH_L^p(\mathbb{R}^n)$. Typical examples of such operators include the $2k$-order divergence form homogeneous elliptic operator $L_1:=(-1)^k\sum_{|α|=k=|β|}\partial^β(a_{α,β}\partial^α)$, where $\{a_{α,β}\}_{|α|=k=|β|}$ are complex bounded measurable functions, and the $2k$-order Schrödinger type operator $L_2:= (-Δ)^k+V^k$, where $Δ$ is the Laplacian operator and $0\le V\in L^k_{\mathop\mathrm{loc}}(\mathbb{R}^n)$. As applications, for $i\in\{1,\,2\}$ and $p\in(\frac{n}{n+k},\,1]$, the authors prove that the associated Riesz transform $\nabla^k (L_i^{-1/2})$ is bounded from $WH^p_{L_i}(\mathbb{R}^n)$ to the classical weak Hardy space $WH^p(\mathbb{R}^n)$ and, for all $0<p<r\le1$ and $α=n(\frac{1}{p}-\frac{1}{r})$, the fractional power $L_i^{-\fracα{2k}}$ is bounded from $WH_{L_i}^p(\mathbb{R}^n)$ to $WH_{L_i}^r(\mathbb{R}^n)$. Furthermore, the authors find the dual space of $WH_L^p(\mathbb{R}^n)$ for $p\in(0,\,1]$, which can be defined via mean oscillations based on some subtle coverings of bounded open sets and, even when $L:=-Δ$, are also previously unknown. In particular, if $L$ is a nonnegative self-adjoint operator in $L^2({\mathbb R}^n)$ satisfying the Davies-Gaffney estimates, the authors further establish the weak atomic characterization of $WH_L^p(\mathbb{R}^n)$.

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