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Brown Halmos Operator Identity and Toeplitz Operators on the Dirichlet Space

Ashish Kujur, Md Ramiz Reza

Abstract

A well known result of Brown and Halmos shows that the Toeplitz operators induced by $L^{\infty}(\mathbb T)$ symbols on the Hardy space of the unit disc $\mathbb D$ are characterized by the operator identity $T_{\bar{z}}AT_z=A,$ where $T_z, T_{\bar{z}}$ are the Toeplitz operators induced by the function $z$ and $\bar{z}$ on the unit circle $\mathbb T$ respectively. In this paper we introduce and study a class of Toeplitz operators on the Dirichlet space $\mathcal{D} _0$ induced by a symbol class $\mathcal T(\mathcal D _0)= \overline{H^{\infty}_0(\mathbb D)} + \mathcal M(\mathcal D_0 ),$ where $H^{\infty}_0(\mathbb D)$ denotes the set of all bounded analytic function on $\mathbb D$ vanishing at $0$ and $\mathcal M(\mathcal D _0)$ denotes the multiplier algebra of the Dirichlet space $\mathcal D_0.$ We find that the Toeplitz operators on the Dirichlet space $\mathcal D$ induced by the symbol class $\mathcal T(\mathcal D _0)$ is completely characterized by the operator identity $T_{\bar{z}}AT_z=A.$

Brown Halmos Operator Identity and Toeplitz Operators on the Dirichlet Space

Abstract

A well known result of Brown and Halmos shows that the Toeplitz operators induced by symbols on the Hardy space of the unit disc are characterized by the operator identity where are the Toeplitz operators induced by the function and on the unit circle respectively. In this paper we introduce and study a class of Toeplitz operators on the Dirichlet space induced by a symbol class where denotes the set of all bounded analytic function on vanishing at and denotes the multiplier algebra of the Dirichlet space We find that the Toeplitz operators on the Dirichlet space induced by the symbol class is completely characterized by the operator identity

Paper Structure

This paper contains 4 sections, 19 theorems, 93 equations.

Key Result

Theorem 1.1

If $T\in \mathcal{B}(\mathcal{D}_0)$ satisfies the identity $T_{\bar{z}}TT_z= T$, then there exists a unique $\psi\in \mathcal{T}({\mathcal{D}_0})$ such that $T=T_{\psi}.$

Theorems & Definitions (35)

  • Theorem 1.1
  • Theorem 2.1
  • proof
  • Corollary 2.2
  • Remark 2.3
  • Remark 2.4
  • Proposition 2.5
  • proof
  • Corollary 2.6
  • Proposition 2.7
  • ...and 25 more