<p>Let <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1923_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="199" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varphi :\ [0,1)\times [0,\infty )\rightarrow [0,\infty ]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>φ</mi> <mo>:</mo> <mspace width="4pt" /> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> <mo>×</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> <mo stretchy="false">→</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation> be a Musielak–Orlicz function and <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1923_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="94" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma ,s\in (0,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>γ</mi> <mo>,</mo> <mi>s</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. In this article, the authors present some sufficient conditions to ensure that the dyadic maximal operator <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1923_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="30" /> </InlineMediaObject> <EquationSource Format="TEX">\(U_{\gamma ,s}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>U</mi> <mrow> <mi>γ</mi> <mo>,</mo> <mi>s</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> is bounded on Musielak–Orlicz spaces <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1923_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^{\varphi }[0,1).\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>φ</mi> </msup> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> As applications, the authors establish the characterizations of Musielak–Orlicz Hardy spaces <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1923_Article_IEq5.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{\varphi }[0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>H</mi> <mi>φ</mi> </msub> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and the boundedness of maximal Fejér operators from <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1923_Article_IEq6.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{\varphi }[0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>H</mi> <mi>φ</mi> </msub> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> to <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1923_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^{\varphi }[0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>φ</mi> </msup> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. Furthermore, the almost everywhere convergence and the norm convergence of Fejér means of Walsh–Fourier series are also obtained. All these results include, as special cases, the essentially optimal conditions for variable exponent Lebesgue spaces, perturbed variable exponent Lebesgue spaces, and double-phase functionals with variable exponent Lebesgue spaces.</p>

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Boundedness of Dyadic Maximal Operators on Musielak–Orlicz Type Spaces and Its Applications

  • Ferenc Weisz,
  • Guangheng Xie,
  • Dachun Yang

摘要

Let \(\varphi :\ [0,1)\times [0,\infty )\rightarrow [0,\infty ]\) φ : [ 0 , 1 ) × [ 0 , ) [ 0 , ] be a Musielak–Orlicz function and \(\gamma ,s\in (0,\infty )\) γ , s ( 0 , ) . In this article, the authors present some sufficient conditions to ensure that the dyadic maximal operator \(U_{\gamma ,s}\) U γ , s is bounded on Musielak–Orlicz spaces \(L^{\varphi }[0,1).\) L φ [ 0 , 1 ) . As applications, the authors establish the characterizations of Musielak–Orlicz Hardy spaces \(H_{\varphi }[0,1)\) H φ [ 0 , 1 ) and the boundedness of maximal Fejér operators from \(H_{\varphi }[0,1)\) H φ [ 0 , 1 ) to \(L^{\varphi }[0,1)\) L φ [ 0 , 1 ) . Furthermore, the almost everywhere convergence and the norm convergence of Fejér means of Walsh–Fourier series are also obtained. All these results include, as special cases, the essentially optimal conditions for variable exponent Lebesgue spaces, perturbed variable exponent Lebesgue spaces, and double-phase functionals with variable exponent Lebesgue spaces.