<p>Let <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10188_Article_IEq1.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="87" /> </InlineMediaObject> <EquationSource Format="TEX">\(b\in L_{\textrm{loc}}^1({\mathbb {R}}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>b</mi> <mo>∈</mo> <msubsup> <mi>L</mi> <mrow> <mtext>loc</mtext> </mrow> <mn>1</mn> </msubsup> <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>. In the present paper, we are concerned on the maximal Calderón commutator which is defined by <Equation ID="Equ93"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10188_Article_Equ93.gif" Format="GIF" Height="45" Rendition="HTML" Resolution="72" Type="Linedraw" Width="420" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} {\mathcal {C}}_\Omega ^* f (x)=\sup _{\varepsilon&gt;0}\bigg |\int _{|x-y|&gt;\epsilon }\left( \frac{\Omega (x-y)}{|x-y|^{n+1}}\right) \big (b(x)-b(y)\big )f(y)dy\bigg |, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msubsup> <mi mathvariant="script">C</mi> <mi mathvariant="normal">Ω</mi> <mo>∗</mo> </msubsup> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <munder> <mo movablelimits="true">sup</mo> <mrow> <mi>ε</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </munder> <mrow> <mo maxsize="2.047em" minsize="2.047em" stretchy="true">|</mo> </mrow> <msub> <mo>∫</mo> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo>-</mo> <mi>y</mi> <mo stretchy="false">|</mo> <mo>&gt;</mo> <mi>ϵ</mi> </mrow> </msub> <mfenced close=")" open="("> <mfrac> <mrow> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>-</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo>-</mo> <mi>y</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> </mfrac> </mfenced> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">(</mo> </mrow> <mi>b</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <mi>b</mi> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">)</mo> </mrow> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <mi>d</mi> <mi>y</mi> <mrow> <mo maxsize="2.047em" minsize="2.047em" stretchy="true">|</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>which plays an important role in the almost every convergence of the Calderón commutator proposed by Calderón. In this paper, we obtain the necessary and sufficient conditions on the function <i>b</i> to guarantee that <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10188_Article_IEq2.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {C}}_\Omega ^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="script">C</mi> <mi mathvariant="normal">Ω</mi> <mo>∗</mo> </msubsup> </math></EquationSource> </InlineEquation> is a bounded operator on <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10188_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p(w)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi>w</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10188_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="83" /> </InlineMediaObject> <EquationSource Format="TEX">\(1&lt;p&lt;\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10188_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="59" /> </InlineMediaObject> <EquationSource Format="TEX">\(w\in A_p.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>w</mi> <mo>∈</mo> <msub> <mi>A</mi> <mi>p</mi> </msub> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation></p>

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The characterization for the quantitative weighted bounds of the maximal Calderón commutator with rough kernel

  • Yanping Chen

摘要

Let \(b\in L_{\textrm{loc}}^1({\mathbb {R}}^n)\) b L loc 1 ( R n ) . In the present paper, we are concerned on the maximal Calderón commutator which is defined by \(\begin{aligned} {\mathcal {C}}_\Omega ^* f (x)=\sup _{\varepsilon>0}\bigg |\int _{|x-y|>\epsilon }\left( \frac{\Omega (x-y)}{|x-y|^{n+1}}\right) \big (b(x)-b(y)\big )f(y)dy\bigg |, \end{aligned}\) C Ω f ( x ) = sup ε > 0 | | x - y | > ϵ Ω ( x - y ) | x - y | n + 1 ( b ( x ) - b ( y ) ) f ( y ) d y | , which plays an important role in the almost every convergence of the Calderón commutator proposed by Calderón. In this paper, we obtain the necessary and sufficient conditions on the function b to guarantee that \({\mathcal {C}}_\Omega ^*\) C Ω is a bounded operator on \(L^p(w)\) L p ( w ) for \(1<p<\infty \) 1 < p < and \(w\in A_p.\) w A p .