<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(q\in [1,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>1</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(d\in \{0,1,\ldots \}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>∈</mo> <mo stretchy="false">{</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo>,</mo> <mo>…</mo> <mo stretchy="false">}</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\theta _0\in (0,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, <i>A</i> be a general expansive matrix, and <i>X</i> be a ball quasi-Banach function space on <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({\mathbb {R}}^n\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </math></EquationSource> </InlineEquation> satisfying some mild assumptions. In this article, the authors first introduce the modified anisotropic Calderón–Zygmund operator <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\widetilde{T}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover accent="true"> <mi>T</mi> <mo stretchy="true">~</mo> </mover> </math></EquationSource> </InlineEquation> of the anisotropic Calderón–Zygmund operator <i>T</i>. Then the authors prove that <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\widetilde{T}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover accent="true"> <mi>T</mi> <mo stretchy="true">~</mo> </mover> </math></EquationSource> </InlineEquation> is bounded on the ball anisotropic Campanato-type function space <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="MediaObjects/43034_2026_498_IEq7_HTML.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="120" Type="Linedraw" Width="95" /> </InlineMediaObject> </InlineEquation> if and only if <i>T</i> satisfies the well-known vanishing condition that <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(T^*(x^{\gamma })=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>T</mi> <mo>∗</mo> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mi>x</mi> <mi>γ</mi> </msup> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. Moreover, the authors show that <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\widetilde{T}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover accent="true"> <mi>T</mi> <mo stretchy="true">~</mo> </mover> </math></EquationSource> </InlineEquation> is just the adjoint operator of <i>T</i> on Hardy-type space <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(H_X^A(\mathbb {R}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>X</mi> <mi>A</mi> </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> [the predual space of <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="MediaObjects/43034_2026_498_IEq11_HTML.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="120" Type="Linedraw" Width="95" /> </InlineMediaObject> </InlineEquation>], which strengthens the rationality of the definition of <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\widetilde{T}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover accent="true"> <mi>T</mi> <mo stretchy="true">~</mo> </mover> </math></EquationSource> </InlineEquation>. All these results are new even when they are applied, respectively, to anisotropic weighted Lebesgue spaces, variable Lebesgue spaces, Orlicz spaces, mixed-norm Lebesgue spaces, and Lorentz spaces. To obtain these results, the authors fully use the duality <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="MediaObjects/43034_2026_498_IEq13_HTML.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="120" Type="Linedraw" Width="194" /> </InlineMediaObject> </InlineEquation>, atomic characterizations of <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(H_X^A(\mathbb {R}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>X</mi> <mi>A</mi> </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>, and a specific method for decomposing molecules into a summation of atoms.</p>

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Boundedness of modified anisotropic Calderón–Zygmund operators on anisotropic ball Campanato function spaces

  • Hongchao Jia,
  • Xianjie Yan

摘要

Let \(q\in [1,\infty )\) q [ 1 , ) , \(d\in \{0,1,\ldots \}\) d { 0 , 1 , } , \(\theta _0\in (0,\infty )\) θ 0 ( 0 , ) , A be a general expansive matrix, and X be a ball quasi-Banach function space on \({\mathbb {R}}^n\) R n satisfying some mild assumptions. In this article, the authors first introduce the modified anisotropic Calderón–Zygmund operator \(\widetilde{T}\) T ~ of the anisotropic Calderón–Zygmund operator T. Then the authors prove that \(\widetilde{T}\) T ~ is bounded on the ball anisotropic Campanato-type function space if and only if T satisfies the well-known vanishing condition that \(T^*(x^{\gamma })=0\) T ( x γ ) = 0 . Moreover, the authors show that \(\widetilde{T}\) T ~ is just the adjoint operator of T on Hardy-type space \(H_X^A(\mathbb {R}^n)\) H X A ( R n ) [the predual space of ], which strengthens the rationality of the definition of \(\widetilde{T}\) T ~ . All these results are new even when they are applied, respectively, to anisotropic weighted Lebesgue spaces, variable Lebesgue spaces, Orlicz spaces, mixed-norm Lebesgue spaces, and Lorentz spaces. To obtain these results, the authors fully use the duality , atomic characterizations of \(H_X^A(\mathbb {R}^n)\) H X A ( R n ) , and a specific method for decomposing molecules into a summation of atoms.