On the chaoticity of some tensor product weighted backward shift operators acting on some tensor product Fock-Bargmann spaces

preprint2014arXivOpen access

Abstract

In Advances in Mathematical Physics (2011) we showed that the weighted shift zpdp+1dzp+1z^{p}\frac{d^{p+1}}{dz^{p+1}} (p=0,1,2,...)(p=0, 1, 2, ...) acting on classical Bargmann space Bp\mathbb{B}_{p} is chaotic operator. In Journal of Mathematical physics (2014), we constructed an chaotic weighted shift M∗pMp+1\mathbb{M}^{*^{p}}\mathbb{M}^{p+1} (p=0,1,2,...)(p=0, 1, 2, ...) on some lattice Fock-Bargmann Epα\mathbb{E}_{p}^α generated by the orthonormal basis em(α,p)(z)=emα;m=p,p+1,...e_{m}^{(α,p)}(z) = e_{m}^α ; m=p, p+1, ... where emα(z)=(2νπ)1/4eν2z2e−π2ν(m+α)2+2iπ(m+α)z;m∈Ne_{m}^α(z) = (\frac{2ν}π)^{1/4}e^{\fracν{2}z^{2}}e^{-\frac{π^{2}}ν(m +α)^{2} +2iπ(m +α)z}; m \in \mathbb{N} with ν,αν, α are real numbers; ν>0ν> 0, M\mathbb{M} is an weighted shift and M∗\mathbb{M^{*}} is the adjoint of the M\mathbb{M}. In this paper we study the chaoticity of tensor product M∗pMp+1⊗zpdpdzp+1\mathbb{M}^{*^{p}}\mathbb{M}^{p+1}\otimes z^{p}\frac{d^{p}}{dz^{p+1}} (p=0,1,2,...)(p=0, 1, 2, ...) acting on Epα⊗Bp\mathbb{E}_{p}^α\otimes \mathbb{B}_{p}.

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