<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\varphi : \mathbb {R}^{n}\times [0,\infty )\rightarrow [0,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>φ</mi> <mo>:</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo>×</mo> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">→</mo> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> be a Musielak-Orlicz function satisfying the uniformly anisotropic Muckenhoupt condition and be of uniformly lower type <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(p^-_{\varphi }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>p</mi> <mi>φ</mi> <mo>-</mo> </msubsup> </math></EquationSource> </InlineEquation> and of uniformly upper type <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(p^+_{\varphi }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>p</mi> <mi>φ</mi> <mo>+</mo> </msubsup> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(0&lt;p^-_{\varphi }\le p^+_{\varphi }&lt;\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <msubsup> <mi>p</mi> <mi>φ</mi> <mo>-</mo> </msubsup> <mo>≤</mo> <msubsup> <mi>p</mi> <mi>φ</mi> <mo>+</mo> </msubsup> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(q\in (0,\infty ]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation>, and <i>A</i> be a general expansive matrix on <InlineEquation ID="IEq6"> <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>. In this paper, the authors first study the anisotropic Musielak-Orlicz-Lorentz Hardy space <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(H^{\varphi ,q}_A(\mathbb {R}^{n})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>A</mi> <mrow> <mi>φ</mi> <mo>,</mo> <mi>q</mi> </mrow> </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>, which coincides with the known anisotropic weak Musielak-Orlicz Hardy space <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(H^{\varphi ,\infty }_A(\mathbb {R}^{n})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>A</mi> <mrow> <mi>φ</mi> <mo>,</mo> <mi>∞</mi> </mrow> </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> when <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(q=\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>=</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>, and then establish their atomic and molecular decompositions. As some applications, the authors obtain the boundedness of anisotropic Calderón-Zygmund operators on <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(H^{\varphi ,q}_A(\mathbb {R}^{n})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>A</mi> <mrow> <mi>φ</mi> <mo>,</mo> <mi>q</mi> </mrow> </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> when <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(q\in (0,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and from the anisotropic Musielak-Orlicz Hardy space <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(H^{\varphi }_A(\mathbb {R}^{n})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>A</mi> <mi>φ</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> to <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(H^{\varphi ,\infty }_A(\mathbb {R}^{n})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>A</mi> <mrow> <mi>φ</mi> <mo>,</mo> <mi>∞</mi> </mrow> </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 critical case. All the ranges of the exponents considered are shown to be the best possible, significantly improving upon existing results for <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(H^{\varphi ,\infty }_A(\mathbb {R}^{n})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>A</mi> <mrow> <mi>φ</mi> <mo>,</mo> <mi>∞</mi> </mrow> </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> via widening the original assumption <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(0&lt;p^-_{\varphi }\le p^+_{\varphi }\le 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <msubsup> <mi>p</mi> <mi>φ</mi> <mo>-</mo> </msubsup> <mo>≤</mo> <msubsup> <mi>p</mi> <mi>φ</mi> <mo>+</mo> </msubsup> <mo>≤</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> into the full range <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(0&lt;p^-_{\varphi }\le p^+_{\varphi }&lt;\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <msubsup> <mi>p</mi> <mi>φ</mi> <mo>-</mo> </msubsup> <mo>≤</mo> <msubsup> <mi>p</mi> <mi>φ</mi> <mo>+</mo> </msubsup> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>, and all the results for <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(q\in (0,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> are novel and generalize from isotropic setting to anisotropic frameworks.</p>

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Real-Variable Theory of Anisotropic Musielak-Orlicz-Lorentz Hardy Spaces with Applications to Calderón-Zygmund Operators

  • Xiong Liu,
  • Wenhua Wang

摘要

Let \(\varphi : \mathbb {R}^{n}\times [0,\infty )\rightarrow [0,\infty )\) φ : R n × [ 0 , ) [ 0 , ) be a Musielak-Orlicz function satisfying the uniformly anisotropic Muckenhoupt condition and be of uniformly lower type \(p^-_{\varphi }\) p φ - and of uniformly upper type \(p^+_{\varphi }\) p φ + with \(0<p^-_{\varphi }\le p^+_{\varphi }<\infty \) 0 < p φ - p φ + < , \(q\in (0,\infty ]\) q ( 0 , ] , and A be a general expansive matrix on \(\mathbb {R}^{n}\) R n . In this paper, the authors first study the anisotropic Musielak-Orlicz-Lorentz Hardy space \(H^{\varphi ,q}_A(\mathbb {R}^{n})\) H A φ , q ( R n ) , which coincides with the known anisotropic weak Musielak-Orlicz Hardy space \(H^{\varphi ,\infty }_A(\mathbb {R}^{n})\) H A φ , ( R n ) when \(q=\infty \) q = , and then establish their atomic and molecular decompositions. As some applications, the authors obtain the boundedness of anisotropic Calderón-Zygmund operators on \(H^{\varphi ,q}_A(\mathbb {R}^{n})\) H A φ , q ( R n ) when \(q\in (0,\infty )\) q ( 0 , ) and from the anisotropic Musielak-Orlicz Hardy space \(H^{\varphi }_A(\mathbb {R}^{n})\) H A φ ( R n ) to \(H^{\varphi ,\infty }_A(\mathbb {R}^{n})\) H A φ , ( R n ) in the critical case. All the ranges of the exponents considered are shown to be the best possible, significantly improving upon existing results for \(H^{\varphi ,\infty }_A(\mathbb {R}^{n})\) H A φ , ( R n ) via widening the original assumption \(0<p^-_{\varphi }\le p^+_{\varphi }\le 1\) 0 < p φ - p φ + 1 into the full range \(0<p^-_{\varphi }\le p^+_{\varphi }<\infty \) 0 < p φ - p φ + < , and all the results for \(q\in (0,\infty )\) q ( 0 , ) are novel and generalize from isotropic setting to anisotropic frameworks.