<p>The kernel of a Toeplitz operator is nearly <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="20_2025_2797_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(S^{*}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mi>S</mi> <mrow /> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>-invariant where <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="20_2025_2797_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(S^{*}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mi>S</mi> <mrow /> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> is the backward shift on the Hardy space of the unit disk. Recently, the question when the kernel of a finite rank perturbation of a Toeplitz operator is nearly <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="20_2025_2797_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(S^{*}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mi>S</mi> <mrow /> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>-invariant with finite defect is studied in Liang and Partington (Integral Equ Oper Theory 92, Paper No. 35, 2020) where the multiplicity of <i>S</i> is one and in Chattopadhyay et al. (Adv. Oper. Theory 6, Paper No. 49, 2021) where the multiplicity of <i>S</i> is finite. This question is answered affirmatively for several important classes of Toeplitz operators in Liang and Partington (2020), Chattopadhyay et al. (2021). In this paper we give a complete answer to this question even when <i>S</i> is of infinite multiplicity. Furthermore, our approach is general enough to cover related questions on almost <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="20_2025_2797_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(S^{*}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mi>S</mi> <mrow /> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>-invariant and almost <i>S</i>-invariant kernels and to include related operators such as Hankel operators and product of Toeplitz and Hankel operators.</p>

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Almost Backward Shift Invariance of Kernels of Perturbed Toeplitz and Hankel Operators

  • Caixing Gu

摘要

The kernel of a Toeplitz operator is nearly \(S^{*}\) S -invariant where \(S^{*}\) S is the backward shift on the Hardy space of the unit disk. Recently, the question when the kernel of a finite rank perturbation of a Toeplitz operator is nearly \(S^{*}\) S -invariant with finite defect is studied in Liang and Partington (Integral Equ Oper Theory 92, Paper No. 35, 2020) where the multiplicity of S is one and in Chattopadhyay et al. (Adv. Oper. Theory 6, Paper No. 49, 2021) where the multiplicity of S is finite. This question is answered affirmatively for several important classes of Toeplitz operators in Liang and Partington (2020), Chattopadhyay et al. (2021). In this paper we give a complete answer to this question even when S is of infinite multiplicity. Furthermore, our approach is general enough to cover related questions on almost \(S^{*}\) S -invariant and almost S-invariant kernels and to include related operators such as Hankel operators and product of Toeplitz and Hankel operators.