Abstract
In this paper, we consider the Schrödinger operators \(L_k=-\Delta _k+V\), where \(\Delta _k\) is the Dunkl–Laplace operator and V is a non-negative potential on \(\mathbb {R}^d\). We establish that \(L_k \) is essentially self-adjoint on \(C_0^\infty (\mathbb {R}^d)\). In particular, we develop a bounded \(H^\infty \)-calculus on \(L^p\) spaces for the Dunkl harmonic oscillator operator.
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The authors would like to express their sincere thanks to the referee for his comments and suggestions.
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Communicated by Daniel Aron Alpay.
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Amri, B., Hammi, A. Dunkl–Schrödinger Operators. Complex Anal. Oper. Theory 13, 1033–1058 (2019). https://doi.org/10.1007/s11785-018-0834-1
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DOI: https://doi.org/10.1007/s11785-018-0834-1