<p>We work in the general framework of a family of singular integrals with kernels controlled in terms of a critical radius function <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\rho \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> </InlineEquation>. This family models the harmonic analysis derived from the Schrödinger operator <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(L= -\Delta +V\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>L</mi> <mo>=</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo>+</mo> <mi>V</mi> </mrow> </math></EquationSource> </InlineEquation>, where the non-negative potential <i>V</i> satisfies an appropriate reverse Hölder condition. For their commutators, we find sufficient conditions on the symbols for boundedness and/or compactness when acting on weighted <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation> spaces. In all cases, the classes of symbols and weights are larger than their classical counterparts, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(BMO \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="italic">BMO</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(CMO \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="italic">CMO</mi> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(A_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>A</mi> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>. When these general results are applied to the Schrödinger context, we obtain boundedness and compactness for commutators of operators like <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\nabla L^{-1/2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">∇</mi> <msup> <mi>L</mi> <mrow> <mo>-</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\nabla ^2 L^{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi mathvariant="normal">∇</mi> <mn>2</mn> </msup> <msup> <mi>L</mi> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(V^{1/2} L^{-1/2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>V</mi> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </msup> <msup> <mi>L</mi> <mrow> <mo>-</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(V^{1/2} \nabla L^{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>V</mi> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </msup> <mi mathvariant="normal">∇</mi> <msup> <mi>L</mi> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(V L^{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <msup> <mi>L</mi> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(L^{i\alpha }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mrow> <mi>i</mi> <mi>α</mi> </mrow> </msup> </math></EquationSource> </InlineEquation>. As in Uchiyama’s classical paper, we give a full description of the class for compactness, <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(CMO ^\infty _\rho \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>M</mi> <msubsup> <mi>O</mi> <mi>ρ</mi> <mi>∞</mi> </msubsup> </mrow> </math></EquationSource> </InlineEquation>, under mild conditions on <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\rho \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> </InlineEquation>. Finally, we provide examples showing that <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(CMO \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="italic">CMO</mi> </mrow> </math></EquationSource> </InlineEquation> is strictly contained in <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(CMO ^\infty _\rho \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>M</mi> <msubsup> <mi>O</mi> <mi>ρ</mi> <mi>∞</mi> </msubsup> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Boundedness and Compactness for Commutators of Singular Integrals Related to a Critical Radius Function

  • B. Bongioanni,
  • E. Harboure,
  • P. Quijano

摘要

We work in the general framework of a family of singular integrals with kernels controlled in terms of a critical radius function \(\rho \) ρ . This family models the harmonic analysis derived from the Schrödinger operator \(L= -\Delta +V\) L = - Δ + V , where the non-negative potential V satisfies an appropriate reverse Hölder condition. For their commutators, we find sufficient conditions on the symbols for boundedness and/or compactness when acting on weighted \(L^p\) L p spaces. In all cases, the classes of symbols and weights are larger than their classical counterparts, \(BMO \) BMO , \(CMO \) CMO and \(A_p\) A p . When these general results are applied to the Schrödinger context, we obtain boundedness and compactness for commutators of operators like \(\nabla L^{-1/2}\) L - 1 / 2 , \(\nabla ^2 L^{-1}\) 2 L - 1 , \(V^{1/2} L^{-1/2}\) V 1 / 2 L - 1 / 2 , \(V^{1/2} \nabla L^{-1}\) V 1 / 2 L - 1 , \(V L^{-1}\) V L - 1 and \(L^{i\alpha }\) L i α . As in Uchiyama’s classical paper, we give a full description of the class for compactness, \(CMO ^\infty _\rho \) C M O ρ , under mild conditions on \(\rho \) ρ . Finally, we provide examples showing that \(CMO \) CMO is strictly contained in \(CMO ^\infty _\rho \) C M O ρ .