<p>In this paper we discuss the boundedness of the Hardy–Littlewood maximal operator <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13324_2025_1020_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="79" /> </InlineMediaObject> <EquationSource Format="TEX">\(M_{\lambda }, \ \lambda \ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>M</mi> <mi>λ</mi> </msub> <mo>,</mo> <mspace width="4pt" /> <mi>λ</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, and the variable Riesz potential operator <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13324_2025_1020_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="92" /> </InlineMediaObject> <EquationSource Format="TEX">\(I_{\alpha (\cdot ),\tau }, \ \tau \ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>I</mi> <mrow> <mi>α</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> <mo>,</mo> <mi>τ</mi> </mrow> </msub> <mo>,</mo> <mspace width="4pt" /> <mi>τ</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, on Musielak–Orlicz–Morrey spaces <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13324_2025_1020_Article_IEq3.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="69" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^{\Phi ,\kappa ,\theta }(X)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mrow> <mi mathvariant="normal">Φ</mi> <mo>,</mo> <mi>κ</mi> <mo>,</mo> <mi>θ</mi> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> over unbounded metric measure spaces <i>X</i>. As an important example, we obtain the boundedness of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13324_2025_1020_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="27" /> </InlineMediaObject> <EquationSource Format="TEX">\(M_{\lambda }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>M</mi> <mi>λ</mi> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13324_2025_1020_Article_IEq5.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(I_{\alpha (\cdot ),\tau }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>I</mi> <mrow> <mi>α</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> <mo>,</mo> <mi>τ</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> in the framework of double phase functionals with variable exponents <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13324_2025_1020_Article_IEq6.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="285" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Phi (x,t) = t^{p(x)} + a(x) t^{q(x)}, \ x \in X, \ t \ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Φ</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msup> <mi>t</mi> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </msup> <mo>+</mo> <mi>a</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mi>t</mi> <mrow> <mi>q</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </msup> <mo>,</mo> <mspace width="4pt" /> <mi>x</mi> <mo>∈</mo> <mi>X</mi> <mo>,</mo> <mspace width="4pt" /> <mi>t</mi> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13324_2025_1020_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="86" /> </InlineMediaObject> <EquationSource Format="TEX">\(p(x)&lt;q(x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mo>&lt;</mo> <mi>q</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13324_2025_1020_Article_IEq8.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\(x\in X\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>∈</mo> <mi>X</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13324_2025_1020_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(a(\cdot )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is a non-negative, bounded and Hölder continuous function of order <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13324_2025_1020_Article_IEq10.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="65" /> </InlineMediaObject> <EquationSource Format="TEX">\(\theta \in (0,1]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>θ</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation>. Our results are new even for the variable exponent Morrey spaces or for the doubling metric measure case in that the underlying spaces need not be bounded.</p>

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Generalized Riesz potential operators on Musielak–Orlicz–Morrey spaces over unbounded metric measure spaces

  • Takao Ohno,
  • Tetsu Shimomura

摘要

In this paper we discuss the boundedness of the Hardy–Littlewood maximal operator \(M_{\lambda }, \ \lambda \ge 1\) M λ , λ 1 , and the variable Riesz potential operator \(I_{\alpha (\cdot ),\tau }, \ \tau \ge 1\) I α ( · ) , τ , τ 1 , on Musielak–Orlicz–Morrey spaces \(L^{\Phi ,\kappa ,\theta }(X)\) L Φ , κ , θ ( X ) over unbounded metric measure spaces X. As an important example, we obtain the boundedness of \(M_{\lambda }\) M λ and \(I_{\alpha (\cdot ),\tau }\) I α ( · ) , τ in the framework of double phase functionals with variable exponents \(\Phi (x,t) = t^{p(x)} + a(x) t^{q(x)}, \ x \in X, \ t \ge 0\) Φ ( x , t ) = t p ( x ) + a ( x ) t q ( x ) , x X , t 0 , where \(p(x)<q(x)\) p ( x ) < q ( x ) for \(x\in X\) x X , \(a(\cdot )\) a ( · ) is a non-negative, bounded and Hölder continuous function of order \(\theta \in (0,1]\) θ ( 0 , 1 ] . Our results are new even for the variable exponent Morrey spaces or for the doubling metric measure case in that the underlying spaces need not be bounded.