English

On semigroups generated by sums of even powers of Dunkl operators

Functional Analysis 2019-06-21 v2

Abstract

On the Euclidean space RN\mathbb R^N equipped with a normalized root system RR, a multiplicity function k0k\geq 0, and the associated measure dw(x)=αRx,αk(α)dxdw(\mathbf x)=\prod_{\alpha\in R} |\langle \mathbf x,\alpha\rangle|^{k(\alpha)}d\mathbf x we consider the differential-difference operator L=(1)+1j=1mTζj2,L=(-1)^{\ell+1} \sum_{j=1}^m T_{\zeta_j}^{2\ell}, where ζ1,...,ζm\zeta_1,...,\zeta_m are nonzero vectors in RN\mathbb R^N, which span RN\mathbb R^N, and TζjT_{\zeta_j} are the Dunkl operators. The operator LL is essentially self-adjoint on L2(dw)L^2(dw) and generates a semigroup {St}t0\{S_t\}_{t \geq 0} of linear self-adjoint contractions, which has the form Stf(x)=fqt(x)S_tf(\mathbf x)=f*q_t(\mathbf{x}), qt(x)=tN/(2)q(x/t1/(2))q_t(\mathbf x)=t^{-\mathbf N/ (2\ell)}q(\mathbf x/ t^{1/ (2\ell)}), where q(x)q(\mathbf x) is the Dunkl transform of the function exp(j=1mζj,ξ2) \exp(-\sum_{j=1}^m \langle \zeta_j,\xi\rangle^{2\ell}). We prove that q(x)q(\mathbf x) satisfies the following exponential decay: q(x)exp(cx2/(21)) |q(\mathbf x)| \lesssim \exp(-c \| \mathbf x\|^{2\ell/ (2\ell-1)}) for a certain constant c>0c>0. Moreover, if q(x,y)=τxq(y)q(\mathbf x,\mathbf y)=\tau_{\mathbf x}q(-\mathbf y), then q(x,y)w(B(x,1))1exp(cd(x,y)2/(21))|q(\mathbf x,\mathbf y)|\lesssim w(B(\mathbf x,1))^{-1} \exp(-c d(\mathbf x,\mathbf y)^{2\ell / (2\ell-1)}), where d(x,y)=minσGxσ(y)d(\mathbf x,\mathbf y)=\min_{\sigma\in G}\| \mathbf x- \sigma(\mathbf y)\| , GG~is the reflection group for RR, and τx\tau_{\mathbf x} denotes the Dunkl translation.

Keywords

Cite

@article{arxiv.1905.07344,
  title  = {On semigroups generated by sums of even powers of Dunkl operators},
  author = {Jacek Dziubański and Agnieszka Hejna},
  journal= {arXiv preprint arXiv:1905.07344},
  year   = {2019}
}

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26 pages