<p>In this work we consider <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="68" /> </InlineMediaObject> <EquationSource Format="TEX">\(X\text {-valued}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>X</mi> <mtext>-valued</mtext> </mrow> </math></EquationSource> </InlineEquation> Lebesgue space (so called Bochner space) <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq8.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="64" /> </InlineMediaObject> <EquationSource Format="TEX">\(L_p(\Gamma ;X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Γ</mi> <mo>;</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="95" /> </InlineMediaObject> <EquationSource Format="TEX">\(1&lt;p&lt;+\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mo>+</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq10.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation> is a closed, simple Lyapunov or Radon curve on complex plane. We introduce the concept of a <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq11.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="48" /> </InlineMediaObject> <EquationSource Format="TEX">\(t\text {-basis}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mtext>-basis</mtext> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq8.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="64" /> </InlineMediaObject> <EquationSource Format="TEX">\(L_p(\Gamma ;X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Γ</mi> <mo>;</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, and investigate systems of generalized Faber polynomials corresponding to the domains <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq13.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\(int\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>i</mi> <mi>n</mi> <mi>t</mi> <mi mathvariant="normal">Γ</mi> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq14.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="35" /> </InlineMediaObject> <EquationSource Format="TEX">\(ext\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>e</mi> <mi>x</mi> <mi>t</mi> <mi mathvariant="normal">Γ</mi> </mrow> </math></EquationSource> </InlineEquation>. Some operators are defined that act from the Hardy-Bochner classes <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq15.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{p}^{\pm }(X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mrow> <mi>p</mi> </mrow> <mo>±</mo> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> to <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq16.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="64" /> </InlineMediaObject> <EquationSource Format="TEX">\(L_{p}(\Gamma ;X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Γ</mi> <mo>;</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, where <i>X</i> is a UMD space. We prove the invertibility of these operators and, using the results of <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(t\text {-basicity}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mtext>-basicity</mtext> </mrow> </math></EquationSource> </InlineEquation> of parts of the exponential system for <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq15.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{p}^{\pm }(X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mrow> <mi>p</mi> </mrow> <mo>±</mo> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> spaces. Additionally, we define the <InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="68" /> </InlineMediaObject> <EquationSource Format="TEX">\(X\text {-valued}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>X</mi> <mtext>-valued</mtext> </mrow> </math></EquationSource> </InlineEquation> Smirnov classes <InlineEquation ID="IEq20"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq20.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="53" /> </InlineMediaObject> <EquationSource Format="TEX">\(E_{p}^{\pm }(X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>E</mi> <mrow> <mi>p</mi> </mrow> <mo>±</mo> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> corresponding to the domains <InlineEquation ID="IEq21"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq13.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\(int\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>i</mi> <mi>n</mi> <mi>t</mi> <mi mathvariant="normal">Γ</mi> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq22"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="25_2025_2525_Article_IEq14.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="35" /> </InlineMediaObject> <EquationSource Format="TEX">\(ext\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>e</mi> <mi>x</mi> <mi>t</mi> <mi mathvariant="normal">Γ</mi> </mrow> </math></EquationSource> </InlineEquation>, respectively. It is proved that Faber polynomials form a <i>t</i>-basis for Smirnov-Faber classes, and using this fact, the <i>t</i>-basisness of double the system of Faber polynomials for Bochner spaces is established. Some properties of Smirnov-Bochner classes are also studied.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

\(X\text {-valued}\) Smirnov classes and \(t\text {-basicity}\) of Faber polynomials

  • B. T. Bilalov,
  • A. Buyukarslan,
  • N. P. Nasibova,
  • S. R. Sadigova

摘要

In this work we consider \(X\text {-valued}\) X -valued Lebesgue space (so called Bochner space) \(L_p(\Gamma ;X)\) L p ( Γ ; X ) , \(1<p<+\infty \) 1 < p < + , where \(\Gamma \) Γ is a closed, simple Lyapunov or Radon curve on complex plane. We introduce the concept of a \(t\text {-basis}\) t -basis for \(L_p(\Gamma ;X)\) L p ( Γ ; X ) , and investigate systems of generalized Faber polynomials corresponding to the domains \(int\Gamma \) i n t Γ and \(ext\Gamma \) e x t Γ . Some operators are defined that act from the Hardy-Bochner classes \(H_{p}^{\pm }(X)\) H p ± ( X ) to \(L_{p}(\Gamma ;X)\) L p ( Γ ; X ) , where X is a UMD space. We prove the invertibility of these operators and, using the results of \(t\text {-basicity}\) t -basicity of parts of the exponential system for \(H_{p}^{\pm }(X)\) H p ± ( X ) spaces. Additionally, we define the \(X\text {-valued}\) X -valued Smirnov classes \(E_{p}^{\pm }(X)\) E p ± ( X ) corresponding to the domains \(int\Gamma \) i n t Γ and \(ext\Gamma \) e x t Γ , respectively. It is proved that Faber polynomials form a t-basis for Smirnov-Faber classes, and using this fact, the t-basisness of double the system of Faber polynomials for Bochner spaces is established. Some properties of Smirnov-Bochner classes are also studied.