The dual of the Hardy space associated to the Dunkl-Schrödinger operator with reverse Hölder class potential
Let $\mathcal{L}_k = -Δ_k + V$ be a Schrödinger operator associated with the Dunkl Laplacian $Δ_k$, where $V$ is the non-negative potential function belonging to the reverse Hölder class $RH_k^q(\mathbb{R}^n)$ with $q> \max\{1, \frac{n+2γ}{2}\}$. Here, $2γ$ denotes the degree of homogeneity of the weight function $w_k$, which is determined by the normalized root system and the non-negative multiplicity function $k$. In this paper, we investigate the dual space of the Hardy space $H_{\Tilde{\mathcal{L}}_k}^1$ associated with the Dunkl-Schrödinger operator. The dual space $BMO(\mathcal{L}_k)$ is a subspace of the $BMO_k$ space, which is the Dunkl analogue of the classical $BMO(\mathcal{L})$ space. We provide a characterization for the $BMO(\mathcal{L}_k)$ space. The duality result is obtained via the atomic decomposition of $H_{\Tilde{\mathcal{L}}_k}^1$, where the cancellation condition of atoms depends on the critical radius function associated with the potential $V$. Finally, we establish the boundedness of the uncentered maximal function on the space $BMO(\mathcal{L}_k)$.