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On Dunkl Schr\"odinger semigroups with Green bounded potentials

Functional Analysis 2022-04-08 v1

Abstract

On RN\mathbb R^N equipped with a normalized root system RR, a multiplicity function k(α)>0k(\alpha) > 0, and the associated measure dw(x)=αRx,αk(α)dx, dw(\mathbf x)=\prod_{\alpha\in R}|\langle \mathbf x,\alpha\rangle|^{k(\alpha)}\, d\mathbf x, we consider a Dunkl Schr\"odinger operator L=Δk+VL=-\Delta_k+V, where Δk\Delta_k is the Dunkl Laplace operator and VLloc1(dw)V\in L^1_{\rm loc} (dw) is a non-negative potential. Let ht(x,y)h_t(\mathbf x,\mathbf y) and kt{V}(x,y)k^{\{V\}}_t(\mathbf x,\mathbf y) denote the Dunkl heat kernel and the integral kernel of the semigroup generated by L-L respectively. We prove that kt{V}(x,y)k^{\{V\}}_t(\mathbf x,\mathbf y) satisfies the following heat kernel lower bounds: there are constants C,c>0C, c>0 such that hct(x,y)Ckt{V}(x,y) h_{ct}(\mathbf x,\mathbf y)\leq C k^{\{V\}}_t(\mathbf x,\mathbf y) if and only if supxRN0RNV(y)w(B(x,t))1exy2/tdw(y)dt<, \sup_{\mathbf x\in\mathbb R^N} \int_0^\infty \int_{\mathbb R^N} V(\mathbf y)w(B(\mathbf x,\sqrt{t}))^{-1}e^{-\|\mathbf x-\mathbf y\|^2/t}\, dw(\mathbf y)\, dt<\infty, where B(x,t)B(\mathbf x,\sqrt{t}) stands for the Euclidean ball centered at xRN\mathbf x \in \mathbb{R}^N and radius t\sqrt{t}.

Keywords

Cite

@article{arxiv.2204.03443,
  title  = {On Dunkl Schr\"odinger semigroups with Green bounded potentials},
  author = {Jacek Dziubański and Agnieszka Hejna},
  journal= {arXiv preprint arXiv:2204.03443},
  year   = {2022}
}

Comments

22 pages

R2 v1 2026-06-24T10:41:11.819Z