<p>It is shown that the classical Bloch space and the Bergman space <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2033_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(A^p_\eta \)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>A</mi> <mi>η</mi> <mi>p</mi> </msubsup> </math></EquationSource> </InlineEquation>, induced by a radial doubling weight <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2033_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\eta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> </InlineEquation>, can be characterized by using the fractional derivative <Equation ID="Equ21"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2033_Article_Equ21.gif" Format="GIF" Height="49" Rendition="HTML" Resolution="72" Type="Linedraw" Width="320" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} f\mapsto R_{\nu ,\omega }(f)(z)=\sum _{k=0}^\infty \frac{\nu _{2k+1}}{\omega _{2k+1}}\widehat{f}(k)z^k,\quad z\in \mathbb {D}, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mi>f</mi> <mo>↦</mo> <msub> <mi>R</mi> <mrow> <mi>ν</mi> <mo>,</mo> <mi>ω</mi> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi>f</mi> <mo stretchy="false">)</mo> </mrow> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <munderover> <mo>∑</mo> <mrow> <mi>k</mi> <mo>=</mo> <mn>0</mn> </mrow> <mi>∞</mi> </munderover> <mfrac> <msub> <mi>ν</mi> <mrow> <mn>2</mn> <mi>k</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <msub> <mi>ω</mi> <mrow> <mn>2</mn> <mi>k</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> </mfrac> <mover accent="true"> <mi>f</mi> <mo stretchy="true">^</mo> </mover> <mrow> <mo stretchy="false">(</mo> <mi>k</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mi>z</mi> <mi>k</mi> </msup> <mo>,</mo> <mspace width="1em" /> <mi>z</mi> <mo>∈</mo> <mi mathvariant="double-struck">D</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>induced by two radial weights admitting certain doubling conditions. Here <Equation ID="Equ22"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2033_Article_Equ22.gif" Format="GIF" Height="44" Rendition="HTML" Resolution="72" Type="Linedraw" Width="177" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \omega _{2k+1}=\int _0^1r^{2k+1}\omega (r)\,dr \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>ω</mi> <mrow> <mn>2</mn> <mi>k</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mo>=</mo> <msubsup> <mo>∫</mo> <mn>0</mn> <mn>1</mn> </msubsup> <msup> <mi>r</mi> <mrow> <mn>2</mn> <mi>k</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> <mi>ω</mi> <mrow> <mo stretchy="false">(</mo> <mi>r</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="0.166667em" /> <mi>d</mi> <mi>r</mi> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>are the odd moments of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2033_Article_IEq3.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ω</mi> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2033_Article_IEq4.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\(\widehat{f}(k)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mover accent="true"> <mi>f</mi> <mo stretchy="true">^</mo> </mover> <mrow> <mo stretchy="false">(</mo> <mi>k</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> stands for the Maclaurin coefficient of the analytic function <i>f</i> in the unit disc <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2033_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">D</mi> </math></EquationSource> </InlineEquation>. The main findings of this paper generalize and complete in part recent results by Moreno, Peláez and de la Rosa [<i>Fractional derivative description of the Bloch space, Potential Anal. 61 (2024), no. 3, 555–571</i>], and Peláez and de la Rosa [<i>Littlewood-Paley inequalities for fractional derivative on Bergman spaces, Ann. Fenn. Math. 47 (2022), no. 2, 1109–1130</i>]. The arguments employed here rely on integral representations via Bergman reproducing kernels of the operator&#xa0;<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2033_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\(R_{\nu ,\omega }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>R</mi> <mrow> <mi>ν</mi> <mo>,</mo> <mi>ω</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> and hence differ from those used in the said papers.</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

Two-Weight Fractional Derivative on Bloch and Bergman Spaces

  • Antti Perälä,
  • Jouni Rättyä,
  • Siyu Wang

摘要

It is shown that the classical Bloch space and the Bergman space \(A^p_\eta \) A η p , induced by a radial doubling weight \(\eta \) η , can be characterized by using the fractional derivative \(\begin{aligned} f\mapsto R_{\nu ,\omega }(f)(z)=\sum _{k=0}^\infty \frac{\nu _{2k+1}}{\omega _{2k+1}}\widehat{f}(k)z^k,\quad z\in \mathbb {D}, \end{aligned}\) f R ν , ω ( f ) ( z ) = k = 0 ν 2 k + 1 ω 2 k + 1 f ^ ( k ) z k , z D , induced by two radial weights admitting certain doubling conditions. Here \(\begin{aligned} \omega _{2k+1}=\int _0^1r^{2k+1}\omega (r)\,dr \end{aligned}\) ω 2 k + 1 = 0 1 r 2 k + 1 ω ( r ) d r are the odd moments of \(\omega \) ω , and \(\widehat{f}(k)\) f ^ ( k ) stands for the Maclaurin coefficient of the analytic function f in the unit disc \(\mathbb {D}\) D . The main findings of this paper generalize and complete in part recent results by Moreno, Peláez and de la Rosa [Fractional derivative description of the Bloch space, Potential Anal. 61 (2024), no. 3, 555–571], and Peláez and de la Rosa [Littlewood-Paley inequalities for fractional derivative on Bergman spaces, Ann. Fenn. Math. 47 (2022), no. 2, 1109–1130]. The arguments employed here rely on integral representations via Bergman reproducing kernels of the operator  \(R_{\nu ,\omega }\) R ν , ω and hence differ from those used in the said papers.