<p>In this paper, we establish the weak factorizations of the Hardy space associated with the Dunkl operator via the bilinear forms of Dunkl–Riesz transforms <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_461_Article_IEq1.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(\{{\mathcal {R}}_{j}\}_{j=1}^{d}.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mrow> <mo stretchy="false">{</mo> <msub> <mi mathvariant="script">R</mi> <mi>j</mi> </msub> <mo stretchy="false">}</mo> </mrow> <mrow> <mi>j</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>d</mi> </msubsup> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> Note that the kernels of <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_461_Article_IEq2.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\{{\mathcal {R}}_{j}\}_{j=1}^{d}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <mo stretchy="false">{</mo> <msub> <mi mathvariant="script">R</mi> <mi>j</mi> </msub> <mo stretchy="false">}</mo> </mrow> <mrow> <mi>j</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>d</mi> </msubsup> </math></EquationSource> </InlineEquation> involve both the Euclidean and the Dunkl metrics, which are not equivalent. As an application, we provide a new proof for the sufficiency of characterization of the <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_461_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\({\textrm{BMO}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>BMO</mtext> </math></EquationSource> </InlineEquation> space associated to the Dunkl operator via the commutators of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_461_Article_IEq1.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(\{{\mathcal {R}}_{j}\}_{j=1}^{d}.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mrow> <mo stretchy="false">{</mo> <msub> <mi mathvariant="script">R</mi> <mi>j</mi> </msub> <mo stretchy="false">}</mo> </mrow> <mrow> <mi>j</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>d</mi> </msubsup> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation></p>

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Weak factorizations for Hardy spaces in the Dunkl setting

  • Qingdong Guo,
  • Wenting Hu

摘要

In this paper, we establish the weak factorizations of the Hardy space associated with the Dunkl operator via the bilinear forms of Dunkl–Riesz transforms \(\{{\mathcal {R}}_{j}\}_{j=1}^{d}.\) { R j } j = 1 d . Note that the kernels of \(\{{\mathcal {R}}_{j}\}_{j=1}^{d}\) { R j } j = 1 d involve both the Euclidean and the Dunkl metrics, which are not equivalent. As an application, we provide a new proof for the sufficiency of characterization of the \({\textrm{BMO}}\) BMO space associated to the Dunkl operator via the commutators of \(\{{\mathcal {R}}_{j}\}_{j=1}^{d}.\) { R j } j = 1 d .