<p>Assume that <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(L_{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(L_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> are nonnegative self-adjoint operators whose associated semigroups <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(e^{-tL_{1}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>e</mi> <mrow> <mo>-</mo> <mi>t</mi> <msub> <mi>L</mi> <mn>1</mn> </msub> </mrow> </msup> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(e^{-tL_{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>e</mi> <mrow> <mo>-</mo> <mi>t</mi> <msub> <mi>L</mi> <mn>2</mn> </msub> </mrow> </msup> </math></EquationSource> </InlineEquation> satisfy the Davies–Gaffney estimates. In this work, we define the product Hardy spaces <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(H^{p}_{L_{1},L_{2}}(\mathbb {R}^{n_{1}}\times \mathbb {R}^{n_{2}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mrow> <msub> <mi>L</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>L</mi> <mn>2</mn> </msub> </mrow> <mi>p</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <msub> <mi>n</mi> <mn>1</mn> </msub> </msup> <mo>×</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <msub> <mi>n</mi> <mn>2</mn> </msub> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(H^{p}_{\sqrt{L_{1}},\sqrt{L_{2}}}(\mathbb {R}^{n_{1}}\times \mathbb {R}^{n_{2}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mrow> <msqrt> <msub> <mi>L</mi> <mn>1</mn> </msub> </msqrt> <mo>,</mo> <msqrt> <msub> <mi>L</mi> <mn>2</mn> </msub> </msqrt> </mrow> <mi>p</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <msub> <mi>n</mi> <mn>1</mn> </msub> </msup> <mo>×</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <msub> <mi>n</mi> <mn>2</mn> </msub> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> associated to operators <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(L_{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(L_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> via the area integrals <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(S_{L_{1},L_{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>S</mi> <mrow> <msub> <mi>L</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>L</mi> <mn>2</mn> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(S_{\sqrt{L_{1}},\sqrt{L_{2}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>S</mi> <mrow> <msqrt> <msub> <mi>L</mi> <mn>1</mn> </msub> </msqrt> <mo>,</mo> <msqrt> <msub> <mi>L</mi> <mn>2</mn> </msub> </msqrt> </mrow> </msub> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(0&lt; p\le 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>p</mi> <mo>≤</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, respectively. We prove that these Hardy spaces defined by the square functions can be characterized in terms of the product atoms.</p>

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An atomic characterization for product Hardy spaces

  • QingQuan Deng,
  • Djalal Eddine Guedjiba

摘要

Assume that \(L_{1}\) L 1 and \(L_{2}\) L 2 are nonnegative self-adjoint operators whose associated semigroups \(e^{-tL_{1}}\) e - t L 1 and \(e^{-tL_{2}}\) e - t L 2 satisfy the Davies–Gaffney estimates. In this work, we define the product Hardy spaces \(H^{p}_{L_{1},L_{2}}(\mathbb {R}^{n_{1}}\times \mathbb {R}^{n_{2}})\) H L 1 , L 2 p ( R n 1 × R n 2 ) and \(H^{p}_{\sqrt{L_{1}},\sqrt{L_{2}}}(\mathbb {R}^{n_{1}}\times \mathbb {R}^{n_{2}})\) H L 1 , L 2 p ( R n 1 × R n 2 ) associated to operators \(L_{1}\) L 1 and \(L_{2}\) L 2 via the area integrals \(S_{L_{1},L_{2}}\) S L 1 , L 2 and \(S_{\sqrt{L_{1}},\sqrt{L_{2}}}\) S L 1 , L 2 for \(0< p\le 1\) 0 < p 1 , respectively. We prove that these Hardy spaces defined by the square functions can be characterized in terms of the product atoms.