<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(({{\mathcal {X}}},\rho ,\mu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">X</mi> <mo>,</mo> <mi>ρ</mi> <mo>,</mo> <mi>μ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> be a space of homogeneous type in the sense of Coifman and Weiss with the upper dimension <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\omega \in (0,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ω</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. Assume that <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(p\in [1,\infty ]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>1</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <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="IEq5"> <EquationSource Format="TEX">\(\epsilon \in (0,1]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϵ</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\alpha \in (-\infty ,\min \{\frac{1}{p},\frac{\epsilon }{\omega }\})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mo>-</mo> <mi>∞</mi> <mo>,</mo> <mo movablelimits="true">min</mo> <mrow> <mo stretchy="false">{</mo> <mfrac> <mn>1</mn> <mi>p</mi> </mfrac> <mo>,</mo> <mfrac> <mi>ϵ</mi> <mi>ω</mi> </mfrac> <mo stretchy="false">}</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. In this article, the authors obtain the boundedness of <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\epsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ϵ</mi> </math></EquationSource> </InlineEquation>-Calderón–Zygmund operators from the special Riesz–Morrey space <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\({RM^{\text {spe}}_{p,q,\alpha }}(\mathcal {X})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mi>R</mi> <msubsup> <mi>M</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>q</mi> <mo>,</mo> <mi>α</mi> </mrow> <mtext>spe</mtext> </msubsup> </mrow> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> to the special John–Nirenberg–Campanato space <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\({JN^{\text {spe}}_{p,q,\alpha }}(\mathcal {X})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>q</mi> <mo>,</mo> <mi>α</mi> </mrow> <mtext>spe</mtext> </msubsup> </mrow> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> via using an equivalent norm of <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\({JN^{\text {spe}}_{p,q,\alpha }}(\mathcal {X})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>q</mi> <mo>,</mo> <mi>α</mi> </mrow> <mtext>spe</mtext> </msubsup> </mrow> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">X</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and the properties of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\epsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ϵ</mi> </math></EquationSource> </InlineEquation>-Calderón–Zygmund kernels. The novelty of these results is that, in the proof of main theorems, the authors get rid of the dependence on the reverse doubling property of <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\mu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>μ</mi> </math></EquationSource> </InlineEquation> by using admissible sequences of balls instead of those with radii <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\{2^k\}_{k\in \mathbb {N}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">{</mo> <msup> <mn>2</mn> <mi>k</mi> </msup> <mo stretchy="false">}</mo> </mrow> <mrow> <mi>k</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> in the classical annulus decomposition method. As applications, the authors also obtain the boundedness of Calderón–Zygmund operators from special Riesz–Morrey spaces to special John–Nirenberg–Campanato spaces on, respectively, <InlineEquation ID="IEq14"> <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> and the homogeneous group <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\mathbb {G}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">G</mi> </math></EquationSource> </InlineEquation>, which makes the results more accurate.</p>

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Boundedness of Calderón–Zygmund Operators from Riesz–Morrey Spaces to John–Nirenberg–Campanato Spaces

  • Chenchen Zhao,
  • Hongchao Jia,
  • Yijia Song,
  • Xianjie Yan

摘要

Let \(({{\mathcal {X}}},\rho ,\mu )\) ( X , ρ , μ ) be a space of homogeneous type in the sense of Coifman and Weiss with the upper dimension \(\omega \in (0,\infty )\) ω ( 0 , ) . Assume that \(p\in [1,\infty ]\) p [ 1 , ] , \(q\in (1,\infty )\) q ( 1 , ) , \(\epsilon \in (0,1]\) ϵ ( 0 , 1 ] , and \(\alpha \in (-\infty ,\min \{\frac{1}{p},\frac{\epsilon }{\omega }\})\) α ( - , min { 1 p , ϵ ω } ) . In this article, the authors obtain the boundedness of \(\epsilon \) ϵ -Calderón–Zygmund operators from the special Riesz–Morrey space \({RM^{\text {spe}}_{p,q,\alpha }}(\mathcal {X})\) R M p , q , α spe ( X ) to the special John–Nirenberg–Campanato space \({JN^{\text {spe}}_{p,q,\alpha }}(\mathcal {X})\) J N p , q , α spe ( X ) via using an equivalent norm of \({JN^{\text {spe}}_{p,q,\alpha }}(\mathcal {X})\) J N p , q , α spe ( X ) and the properties of \(\epsilon \) ϵ -Calderón–Zygmund kernels. The novelty of these results is that, in the proof of main theorems, the authors get rid of the dependence on the reverse doubling property of \(\mu \) μ by using admissible sequences of balls instead of those with radii \(\{2^k\}_{k\in \mathbb {N}}\) { 2 k } k N in the classical annulus decomposition method. As applications, the authors also obtain the boundedness of Calderón–Zygmund operators from special Riesz–Morrey spaces to special John–Nirenberg–Campanato spaces on, respectively, \({\mathbb {R}}^n\) R n and the homogeneous group \(\mathbb {G}\) G , which makes the results more accurate.