<p>On the real line, the Dunkl operators are differential-difference operators associated with the reflection group <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13226_2025_839_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {Z}_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">Z</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> on <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13226_2025_839_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">R</mi> </math></EquationSource> </InlineEquation>. In this paper, for <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13226_2025_839_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>γ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, we prove the boundedness of the Dunkl Bessel Riesz operator <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13226_2025_839_Article_IEq4.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="27" /> </InlineMediaObject> <EquationSource Format="TEX">\(I_{\alpha ,\gamma }^{\nu }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>I</mi> <mrow> <mi>α</mi> <mo>,</mo> <mi>γ</mi> </mrow> <mi>ν</mi> </msubsup> </math></EquationSource> </InlineEquation> from the generalized Lebesgue space <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13226_2025_839_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="76" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^{p}(\mathbb {R},d\mu _{\nu })\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo>,</mo> <mi>d</mi> <msub> <mi>μ</mi> <mi>ν</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> into the generalized Lebesgue space <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13226_2025_839_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="75" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^{q}(\mathbb {R},d\mu _{\nu })\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>q</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo>,</mo> <mi>d</mi> <msub> <mi>μ</mi> <mi>ν</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13226_2025_839_Article_IEq7.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(d\mu _\nu \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <msub> <mi>μ</mi> <mi>ν</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> is the weighted Lebesgue measure on <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13226_2025_839_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">R</mi> </math></EquationSource> </InlineEquation>. Also under appropriate assumptions, we obtain the boundedness of <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13226_2025_839_Article_IEq4.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="27" /> </InlineMediaObject> <EquationSource Format="TEX">\(I_{\alpha ,\gamma }^{\nu }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>I</mi> <mrow> <mi>α</mi> <mo>,</mo> <mi>γ</mi> </mrow> <mi>ν</mi> </msubsup> </math></EquationSource> </InlineEquation> from the Dunkl-type Morrey space <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13226_2025_839_Article_IEq10.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="95" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^{p_1,q_1}(\mathbb {R},d\mu _\nu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mrow> <msub> <mi>p</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>q</mi> <mn>1</mn> </msub> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo>,</mo> <mi>d</mi> <msub> <mi>μ</mi> <mi>ν</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> into Dunkl-type Morrey space <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13226_2025_839_Article_IEq11.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="95" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^{p_2,q_2}(\mathbb {R},d\mu _\nu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mrow> <msub> <mi>p</mi> <mn>2</mn> </msub> <mo>,</mo> <msub> <mi>q</mi> <mn>2</mn> </msub> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo>,</mo> <mi>d</mi> <msub> <mi>μ</mi> <mi>ν</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>.</p>

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The boundedness of Dunkl Bessel Riesz operators on Dunkl-type Morrey spaces

  • Saswata Adhikari,
  • Sanjay Parui

摘要

On the real line, the Dunkl operators are differential-difference operators associated with the reflection group \(\mathbb {Z}_{2}\) Z 2 on \(\mathbb {R}\) R . In this paper, for \(\gamma >0\) γ > 0 , we prove the boundedness of the Dunkl Bessel Riesz operator \(I_{\alpha ,\gamma }^{\nu }\) I α , γ ν from the generalized Lebesgue space \(L^{p}(\mathbb {R},d\mu _{\nu })\) L p ( R , d μ ν ) into the generalized Lebesgue space \(L^{q}(\mathbb {R},d\mu _{\nu })\) L q ( R , d μ ν ) , where \(d\mu _\nu \) d μ ν is the weighted Lebesgue measure on \(\mathbb {R}\) R . Also under appropriate assumptions, we obtain the boundedness of \(I_{\alpha ,\gamma }^{\nu }\) I α , γ ν from the Dunkl-type Morrey space \(L^{p_1,q_1}(\mathbb {R},d\mu _\nu )\) L p 1 , q 1 ( R , d μ ν ) into Dunkl-type Morrey space \(L^{p_2,q_2}(\mathbb {R},d\mu _\nu )\) L p 2 , q 2 ( R , d μ ν ) .