<p>This paper is devoted to studying the behaviors of strongly singular Calderón–Zygmund operators <i>T</i> and their commutators [<i>b</i>,&#xa0;<i>T</i>] generated by <i>T</i> with <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43036_2025_466_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="86" /> </InlineMediaObject> <EquationSource Format="TEX">\(b\in L_{loc}({\mathbb {R}}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>b</mi> <mo>∈</mo> <msub> <mi>L</mi> <mrow> <mi mathvariant="italic">loc</mi> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> on the Musielak–Orlicz Hardy spaces. The authors obtain the boundedness of <i>T</i> from the Musielak–Orlicz Hardy spaces <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43036_2025_466_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(H^\varphi ({\mathbb {R}}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>H</mi> <mi>φ</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> to the Musielak–Orlicz spaces <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43036_2025_466_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^\varphi ({\mathbb {R}}^n),\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>φ</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> and from the Musielak–Orlicz Hardy spaces <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43036_2025_466_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(H^\varphi ({\mathbb {R}}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>H</mi> <mi>φ</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> to themselves if <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43036_2025_466_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="63" /> </InlineMediaObject> <EquationSource Format="TEX">\(T^*1=0.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>T</mi> <mo>∗</mo> </msup> <mn>1</mn> <mo>=</mo> <mn>0</mn> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> Meanwhile, the corresponding mapping properties for the commutators [<i>b</i>,&#xa0;<i>T</i>] are also obtained, provided that <i>b</i> belongs to <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43036_2025_466_Article_IEq6.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="102" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {BMO}_{\varphi ,u}({\mathbb {R}}^n),\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">BMO</mi> <mrow> <mi>φ</mi> <mo>,</mo> <mi>u</mi> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> a non-trivial subspace of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43036_2025_466_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="76" /> </InlineMediaObject> <EquationSource Format="TEX">\({\textrm{BMO}}({\mathbb {R}}^n).\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>BMO</mtext> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation></p>

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Strongly singular Calderón–Zygmund operators and commutators on Musielak–Orlicz Hardy spaces

  • Yanyan Han,
  • Jinghan Shao,
  • Huoxiong Wu

摘要

This paper is devoted to studying the behaviors of strongly singular Calderón–Zygmund operators T and their commutators [bT] generated by T with \(b\in L_{loc}({\mathbb {R}}^n)\) b L loc ( R n ) on the Musielak–Orlicz Hardy spaces. The authors obtain the boundedness of T from the Musielak–Orlicz Hardy spaces \(H^\varphi ({\mathbb {R}}^n)\) H φ ( R n ) to the Musielak–Orlicz spaces \(L^\varphi ({\mathbb {R}}^n),\) L φ ( R n ) , and from the Musielak–Orlicz Hardy spaces \(H^\varphi ({\mathbb {R}}^n)\) H φ ( R n ) to themselves if \(T^*1=0.\) T 1 = 0 . Meanwhile, the corresponding mapping properties for the commutators [bT] are also obtained, provided that b belongs to \(\mathcal {BMO}_{\varphi ,u}({\mathbb {R}}^n),\) BMO φ , u ( R n ) , a non-trivial subspace of \({\textrm{BMO}}({\mathbb {R}}^n).\) BMO ( R n ) .