<p>We initiate the study of vector-valued sub-Bergman spaces on the unit disk, which are de Branges–Rovnyak subspaces of the vector-valued weighted Bergman space <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({A}_{\alpha , E}^{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>A</mi> <mrow> <mi>α</mi> <mo>,</mo> <mi>E</mi> </mrow> <mn>2</mn> </msubsup> </math></EquationSource> </InlineEquation>, defined by the contractions <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(T_{B}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>T</mi> <mi>B</mi> </msub> </math></EquationSource> </InlineEquation> or <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(T_{B}^{*}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mi>T</mi> <mrow> <mi>B</mi> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> for an analytic multiplier <i>B</i> of <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({A}_{\alpha ,E}^{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>A</mi> <mrow> <mi>α</mi> <mo>,</mo> <mi>E</mi> </mrow> <mn>2</mn> </msubsup> </math></EquationSource> </InlineEquation>. There are notable differences between the scalar and vector-valued cases, especially when <i>E</i> is infinite-dimensional. Throughout this work, we fill in some gaps and provide unified proofs for several results from the scalar case. Most of our proofs are more elementary and straightforward.</p>

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Vector-valued sub-Bergman spaces on the unit disk

  • Caixing Gu,
  • Shuaibing Luo,
  • Pan Ma

摘要

We initiate the study of vector-valued sub-Bergman spaces on the unit disk, which are de Branges–Rovnyak subspaces of the vector-valued weighted Bergman space \({A}_{\alpha , E}^{2}\) A α , E 2 , defined by the contractions \(T_{B}\) T B or \(T_{B}^{*}\) T B for an analytic multiplier B of \({A}_{\alpha ,E}^{2}\) A α , E 2 . There are notable differences between the scalar and vector-valued cases, especially when E is infinite-dimensional. Throughout this work, we fill in some gaps and provide unified proofs for several results from the scalar case. Most of our proofs are more elementary and straightforward.