<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\vec {p}\in (0,\infty )^n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mover accent="true"> <mi>p</mi> <mo stretchy="false">→</mo> </mover> <mo>∈</mo> <msup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> <mi>n</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> and <i>A</i> be a general expansive matrix on <InlineEquation ID="IEq2"> <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> with all eigenvalues <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> satisfying <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(|\lambda |&gt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">|</mo> <mi>λ</mi> <mo stretchy="false">|</mo> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>. The anisotropic mixed-norm Hardy spaces <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(H_A^{\vec {p}}(\mathbb {R}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>A</mi> <mover accent="true"> <mi>p</mi> <mo stretchy="false">→</mo> </mover> </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> associated with <i>A</i> were initiated by L. Huang et al. in 2020. In this article, we show the boundedness of area operators from the anisotropic mixed-norm Hardy space <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(H_A^{\vec {p}}(\mathbb {R}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>A</mi> <mover accent="true"> <mi>p</mi> <mo stretchy="false">→</mo> </mover> </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> to the mixed-norm Lebesgue space <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(L^{\vec {p}}(\mathbb {R}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mover accent="true"> <mi>p</mi> <mo stretchy="false">→</mo> </mover> </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> for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\vec {p}\in (1,\infty )^n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mover accent="true"> <mi>p</mi> <mo stretchy="false">→</mo> </mover> <mo>∈</mo> <msup> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> <mi>n</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> in terms of Carleson measures. As an application, we also obtain the boundedness of convolution operators from <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(H_A^{\vec {p}}(\mathbb {R}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>A</mi> <mover accent="true"> <mi>p</mi> <mo stretchy="false">→</mo> </mover> </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> to the tent space <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(T^{\vec {p}}_q(A,\mu _\delta )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>T</mi> <mi>q</mi> <mover accent="true"> <mi>p</mi> <mo stretchy="false">→</mo> </mover> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>A</mi> <mo>,</mo> <msub> <mi>μ</mi> <mi>δ</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\vec {p}\in (1,\infty )^n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mover accent="true"> <mi>p</mi> <mo stretchy="false">→</mo> </mover> <mo>∈</mo> <msup> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> <mi>n</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq12"> <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>, where <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\mu _\delta \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>μ</mi> <mi>δ</mi> </msub> </math></EquationSource> </InlineEquation> is a positive Borel measure on <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\mathbb {R}^n\times \mathbb {Z}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo>×</mo> <mi mathvariant="double-struck">Z</mi> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Area Operators on Anisotropic Mixed-Norm Hardy Spaces via Carleson Measures

  • Guijun Liu,
  • Long Huang,
  • Xiaofeng Wang

摘要

Let \(\vec {p}\in (0,\infty )^n\) p ( 0 , ) n and A be a general expansive matrix on \(\mathbb {R}^n\) R n with all eigenvalues \(\lambda \) λ satisfying \(|\lambda |>1\) | λ | > 1 . The anisotropic mixed-norm Hardy spaces \(H_A^{\vec {p}}(\mathbb {R}^n)\) H A p ( R n ) associated with A were initiated by L. Huang et al. in 2020. In this article, we show the boundedness of area operators from the anisotropic mixed-norm Hardy space \(H_A^{\vec {p}}(\mathbb {R}^n)\) H A p ( R n ) to the mixed-norm Lebesgue space \(L^{\vec {p}}(\mathbb {R}^n)\) L p ( R n ) for \(\vec {p}\in (1,\infty )^n\) p ( 1 , ) n in terms of Carleson measures. As an application, we also obtain the boundedness of convolution operators from \(H_A^{\vec {p}}(\mathbb {R}^n)\) H A p ( R n ) to the tent space \(T^{\vec {p}}_q(A,\mu _\delta )\) T q p ( A , μ δ ) with \(\vec {p}\in (1,\infty )^n\) p ( 1 , ) n and \(q\in [1,\infty )\) q [ 1 , ) , where \(\mu _\delta \) μ δ is a positive Borel measure on \(\mathbb {R}^n\times \mathbb {Z}\) R n × Z .