Weyl's theorem for Toeplitz operators with polynomial symbols on the harmonic Bergman space (Q1995923)
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scientific article; zbMATH DE number 7315658
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Weyl's theorem for Toeplitz operators with polynomial symbols on the harmonic Bergman space |
scientific article; zbMATH DE number 7315658 |
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Weyl's theorem for Toeplitz operators with polynomial symbols on the harmonic Bergman space (English)
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25 February 2021
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Given the unit disk \(\mathbb{D}\) and the normalized Lebesgue area measure \(dA(z)=\frac{1}{\pi}dxdy\), let the harmonic Bergman space \(L^2_h\) be the closed subspace of \(L^2(\mathbb{D},dA)\) consisting of all complex-valued harmonic functions on \(\mathbb{D}\). The Weyl spectrum \(\omega(T)\) of an operator \(T\) is defined by \(\omega(T):=\bigcap_{K\in{\mathcal K}}\sigma(T+K)\), where \(\sigma(T+K)\) denotes the spectrum of \(T+K\) and \({\mathcal K}\) is the set of compact operators. Let \(\pi_{00}(T)\) denote the set of isolated points \(\lambda\in\sigma(T)\) which are eigenvalues of finite geometric multiplicity, i.e., \(0<\dim\ker(T-\lambda I)<\infty\). The authors say that Weyl's theorem holds for an operator \(T\) if \(\omega(T)=\sigma(T)\setminus\pi_{00}(T)\). The Toeplitz operator \(\mathbb{T}_\varphi\) with symbol \(\varphi\in L^\infty(\mathbb{D})\) is defined on the harmonic Bergman space \(L^2_h\) by \(\mathbb{T}_\varphi g=Q(\varphi g)\) for all \(g\in L^2_h\), where \(Q\) is the orthogonal projection of \(L^2(\mathbb{D},dA)\) onto \(L^2_h\). It is proved that Weyl's theorem holds for the Toeplitz operator \(\mathbb{T}_\varphi\) on \(L^2_h\) if \(\varphi\) is any analytic polynomial of degree less than four or \(\varphi(z)=z^n\) for all \(n\in\mathbb{N}\). It was also shown that the spectrum \(\sigma(\mathbb{T}_\varphi)\) can be disconnected for a quadratic polynomial \(\varphi\).
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Toeplitz operator
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harmonic Bergman space
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Weyl's theorem
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0.93321526
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0.93303394
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0.92988694
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0.92220604
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0.9171154
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0.9158596
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0.9142988
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0.91423404
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