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Szeg\"o type limit theorems on the Heisenberg group

Functional Analysis 2022-03-08 v2

Abstract

Let H=ΔH+V\mathcal{H}=-\Delta_{\mathbb{H}}+V be the Schr\"odinger operator on the Heisenberg group Hn\mathbb{H}^n, where ΔH\Delta_{\mathbb{H}} is the full laplacian on Hn\mathbb{H}^n and VV is a positive smooth potential, bounded below and grows like gκ,κ>0|g|^\kappa, \kappa>0 for large g|g|. Let Pr\mathcal{P}_{r} be the orthogonal projection of L2(Hn)L^2(\mathbb{H}^n) onto the space of eigenfunctions of H\mathcal{H} with eigenvalue r\leq r; Let AA be a 0-th order self-adjoint pseudo-differential operator on L2(Hn)L^2(\mathbb{H}^n) relative to the operator 1+λH+V(g),gHn,λR1+|\lambda|H+V(g), g\in \mathbb{H}^n, \lambda \in \mathbb{R}^* with symbol a(g,λ),a(g, {\lambda}), where HH is the Hermite operator on L2(Rn)L^2(\mathbb{R}^n) then \begin{align*} \lim_{r\to\infty} \frac{tr~{f(\mathcal{P}_rA\mathcal{P}_r)}}{tr~(\mathcal{P}_r)} &= \lim_{r\to\infty} \frac{\int_{G^{r}}f(a_{g, {\lambda}}(\xi, x)) \,d\xi\,dx \,dg\,d\mu(\lambda) }{\int_{G^{r}} \,d\xi\,dx \,dg\,d\mu(\lambda)}, \end{align*} (Assuming one limit exists) where Gr={(g,λ,ξ,x)Hn×R×Rn×Rn:λ(1+ξ2+x2)+V(g)r}G^{r}=\{(g, \lambda, \xi, x)\in \mathbb{H}^n \times \mathbb{R}^*\times \mathbb{R}^n\times \mathbb{R}^n : |\lambda |(1+|\xi| ^2+|x|^2)+V(g)\leq r \}, a(g,λ)=OpW(ag,λ)a(g, {\lambda})=Op^W(a_{g, {\lambda}}), and μ(λ)\mu(\lambda) is the Plancherel measure on the Heisenberg group. Also we show that the above limit on the right hand side remains unaltered under a compact perturbation of the pseudo-differential operator AA or a perturbation of the Schr\"odinger operator H\mathcal{H} by bounded self-adjoint operators on L2(Hn)L^2(\mathbb{H}^n).

Keywords

Cite

@article{arxiv.1903.01163,
  title  = {Szeg\"o type limit theorems on the Heisenberg group},
  author = {Shyam Swarup Mondal and Jitendriya Swain},
  journal= {arXiv preprint arXiv:1903.01163},
  year   = {2022}
}

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36 pages