<p>The class of Bounded Oscillation (<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\textrm{BO}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>BO</mtext> </math></EquationSource> </InlineEquation>) operators were introduced and studied by the author in two recent papers. It was shown that many operators in harmonic analysis (Calderón–Zygmund operators, Carleson type operators, martingale transforms, Littlewood-Paley square functions, maximal operators, etc) are <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\textrm{BO}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>BO</mtext> </math></EquationSource> </InlineEquation> operators. <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\textrm{BO}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>BO</mtext> </math></EquationSource> </InlineEquation> operators are defined on abstract measure spaces equipped with a basis of abstract balls. The abstract balls in their definition owe four basic properties of classical balls in <InlineEquation ID="IEq4"> <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>, which are crucial in the study of singular operators on <InlineEquation ID="IEq5"> <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>. Among the various properties of BO operators established in those papers, it was also proved that <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\textrm{BO}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>BO</mtext> </math></EquationSource> </InlineEquation> operators admit pointwise sparse domination, establishing the <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(A_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>A</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation>-conjecture for those operators. In the present paper we study boundedness properties of <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\textrm{BO}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>BO</mtext> </math></EquationSource> </InlineEquation> operators on <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\textrm{BMO }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>BMO</mtext> <mspace width="0.333333em" /> </mrow> </math></EquationSource> </InlineEquation> spaces. In particular, we prove that general <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\textrm{BO}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>BO</mtext> </math></EquationSource> </InlineEquation> operators boundedly map <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(L^\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>∞</mi> </msup> </math></EquationSource> </InlineEquation> into <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\textrm{BMO }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>BMO</mtext> <mspace width="0.333333em" /> </mrow> </math></EquationSource> </InlineEquation>, and under a logarithmic localization condition those map <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\textrm{BMO }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>BMO</mtext> <mspace width="0.333333em" /> </mrow> </math></EquationSource> </InlineEquation> into itself. We obtain these properties as corollaries of new local type bounds, involving oscillations of functions over the balls. We apply the results in the <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\textrm{BMO }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>BMO</mtext> <mspace width="0.333333em" /> </mrow> </math></EquationSource> </InlineEquation> estimations of Calderón–Zygmund operators, martingale transforms, Carleson type operators, as well as in the unconditional basis properties of general wavelet type systems in atomic Hardy spaces <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(H^1\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>H</mi> <mn>1</mn> </msup> </math></EquationSource> </InlineEquation>.</p>

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Bounded oscillation operators on BMO spaces

  • Grigori A. Karagulyan

摘要

The class of Bounded Oscillation ( \(\textrm{BO}\) BO ) operators were introduced and studied by the author in two recent papers. It was shown that many operators in harmonic analysis (Calderón–Zygmund operators, Carleson type operators, martingale transforms, Littlewood-Paley square functions, maximal operators, etc) are \(\textrm{BO}\) BO operators. \(\textrm{BO}\) BO operators are defined on abstract measure spaces equipped with a basis of abstract balls. The abstract balls in their definition owe four basic properties of classical balls in \({\mathbb {R}}^n\) R n , which are crucial in the study of singular operators on \({\mathbb {R}}^n\) R n . Among the various properties of BO operators established in those papers, it was also proved that \(\textrm{BO}\) BO operators admit pointwise sparse domination, establishing the \(A_2\) A 2 -conjecture for those operators. In the present paper we study boundedness properties of \(\textrm{BO}\) BO operators on \(\textrm{BMO }\) BMO spaces. In particular, we prove that general \(\textrm{BO}\) BO operators boundedly map \(L^\infty \) L into \(\textrm{BMO }\) BMO , and under a logarithmic localization condition those map \(\textrm{BMO }\) BMO into itself. We obtain these properties as corollaries of new local type bounds, involving oscillations of functions over the balls. We apply the results in the \(\textrm{BMO }\) BMO estimations of Calderón–Zygmund operators, martingale transforms, Carleson type operators, as well as in the unconditional basis properties of general wavelet type systems in atomic Hardy spaces \(H^1\) H 1 .