<p>For <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ϕ</mi> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\psi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ψ</mi> </math></EquationSource> </InlineEquation> inner functions that fix the origin on the open unit disk <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mathbb {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">D</mi> </math></EquationSource> </InlineEquation> in the complex plane, we consider the question of whether the associated linear operator <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(C_{\phi }^*C_{\psi }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>C</mi> <mrow> <mi>ϕ</mi> </mrow> <mo>∗</mo> </msubsup> <msub> <mi>C</mi> <mi>ψ</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> can be compact or finite-rank on <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(H^2(\mathbb {D})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>H</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">D</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. We show that <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(C_{\phi }^*C_{\psi }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>C</mi> <mrow> <mi>ϕ</mi> </mrow> <mo>∗</mo> </msubsup> <msub> <mi>C</mi> <mi>ψ</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> cannot be rank-one when <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ϕ</mi> </math></EquationSource> </InlineEquation> has purely atomic Aleksandrov–Clark measure and <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\psi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ψ</mi> </math></EquationSource> </InlineEquation> extends continuously to the boundary of <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\mathbb {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">D</mi> </math></EquationSource> </InlineEquation>. When <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ϕ</mi> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\psi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ψ</mi> </math></EquationSource> </InlineEquation> are finite Blaschke products each with two distinct factors, we show <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(C_{\phi }^*C_{\psi }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>C</mi> <mrow> <mi>ϕ</mi> </mrow> <mo>∗</mo> </msubsup> <msub> <mi>C</mi> <mi>ψ</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> cannot be compact. Finally, following work of Cowen and MacCluer, we characterize the range of <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(C_{\phi }^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>C</mi> <mrow> <mi>ϕ</mi> </mrow> <mo>∗</mo> </msubsup> </math></EquationSource> </InlineEquation> when <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(\phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ϕ</mi> </math></EquationSource> </InlineEquation> is a Blaschke product.</p>

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The operator \(C_{\phi }^*C_{\psi }\) when \(\phi \) is a Blaschke product

  • John H. Clifford,
  • Michael Dabkowski,
  • Alan Wiggins,
  • Yunus Zeytuncu

摘要

For \(\phi \) ϕ and \(\psi \) ψ inner functions that fix the origin on the open unit disk \(\mathbb {D}\) D in the complex plane, we consider the question of whether the associated linear operator \(C_{\phi }^*C_{\psi }\) C ϕ C ψ can be compact or finite-rank on \(H^2(\mathbb {D})\) H 2 ( D ) . We show that \(C_{\phi }^*C_{\psi }\) C ϕ C ψ cannot be rank-one when \(\phi \) ϕ has purely atomic Aleksandrov–Clark measure and \(\psi \) ψ extends continuously to the boundary of \(\mathbb {D}\) D . When \(\phi \) ϕ and \(\psi \) ψ are finite Blaschke products each with two distinct factors, we show \(C_{\phi }^*C_{\psi }\) C ϕ C ψ cannot be compact. Finally, following work of Cowen and MacCluer, we characterize the range of \(C_{\phi }^*\) C ϕ when \(\phi \) ϕ is a Blaschke product.