<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math> <mi>T</mi> <mo stretchy="false">(</mo> <mi>f</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$T(f)$</EquationSource> </InlineEquation> denote the Littlewood–Paley square operators, including the Littlewood–Paley <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math> <mi mathvariant="script">G</mi> </math></EquationSource> <EquationSource Format="TEX">$\mathcal{G}$</EquationSource> </InlineEquation>-function <InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math> <mi mathvariant="script">G</mi> <mo stretchy="false">(</mo> <mi>f</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathcal{G}(f)$</EquationSource> </InlineEquation>, Lusin’s area integral <InlineEquation ID="IEq4"> <EquationSource Format="MATHML"><math> <mi mathvariant="script">S</mi> <mo stretchy="false">(</mo> <mi>f</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathcal{S}(f)$</EquationSource> </InlineEquation> and Stein’s function <InlineEquation ID="IEq5"> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="script">G</mi> <mi>λ</mi> <mo>∗</mo> </msubsup> <mo stretchy="false">(</mo> <mi>f</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathcal{G}^{\ast}_{\lambda}(f)$</EquationSource> </InlineEquation> with <InlineEquation ID="IEq6"> <EquationSource Format="MATHML"><math> <mi>λ</mi> <mo>&gt;</mo> <mn>2</mn> </math></EquationSource> <EquationSource Format="TEX">$\lambda &gt;2$</EquationSource> </InlineEquation>. We establish the boundedness of Littlewood–Paley square operators on the weighted spaces <InlineEquation ID="IEq7"> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">BMO</mi> <mo stretchy="false">(</mo> <mi>ω</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathrm{BMO}(\omega )$</EquationSource> </InlineEquation> with <InlineEquation ID="IEq8"> <EquationSource Format="MATHML"><math> <mi>ω</mi> <mo>∈</mo> <msub> <mi>A</mi> <mn>1</mn> </msub> </math></EquationSource> <EquationSource Format="TEX">$\omega \in A_{1}$</EquationSource> </InlineEquation>. The weighted space <InlineEquation ID="IEq9"> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">BLO</mi> <mo stretchy="false">(</mo> <mi>ω</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathrm{BLO}(\omega )$</EquationSource> </InlineEquation> (the space of functions with bounded lower oscillation) is introduced and studied in this paper. This new space is a proper subspace of <InlineEquation ID="IEq10"> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">BMO</mi> <mo stretchy="false">(</mo> <mi>ω</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathrm{BMO}(\omega )$</EquationSource> </InlineEquation>. It is proved that if <InlineEquation ID="IEq11"> <EquationSource Format="MATHML"><math> <mi>T</mi> <mo stretchy="false">(</mo> <mi>f</mi> <mo stretchy="false">)</mo> <mo stretchy="false">(</mo> <msub> <mi>x</mi> <mn>0</mn> </msub> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$T(f)(x_{0})$</EquationSource> </InlineEquation> is finite for a single point <InlineEquation ID="IEq12"> <EquationSource Format="MATHML"><math> <msub> <mi>x</mi> <mn>0</mn> </msub> <mo>∈</mo> <msup> <mi mathvariant="double-struck">R</mi> <mi>n</mi> </msup> </math></EquationSource> <EquationSource Format="TEX">$x_{0}\in \mathbb{R}^{n}$</EquationSource> </InlineEquation>, then <InlineEquation ID="IEq13"> <EquationSource Format="MATHML"><math> <mi>T</mi> <mo stretchy="false">(</mo> <mi>f</mi> <mo stretchy="false">)</mo> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$T(f)(x)$</EquationSource> </InlineEquation> is finite almost everywhere in <InlineEquation ID="IEq14"> <EquationSource Format="MATHML"><math> <msup> <mi mathvariant="double-struck">R</mi> <mi>n</mi> </msup> </math></EquationSource> <EquationSource Format="TEX">$\mathbb{R}^{n}$</EquationSource> </InlineEquation>. Moreover, it is shown that <InlineEquation ID="IEq15"> <EquationSource Format="MATHML"><math> <mi>T</mi> <mo stretchy="false">(</mo> <mi>f</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$T(f)$</EquationSource> </InlineEquation> is bounded from <InlineEquation ID="IEq16"> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">BMO</mi> <mo stretchy="false">(</mo> <mi>ω</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathrm{BMO}(\omega )$</EquationSource> </InlineEquation> into <InlineEquation ID="IEq17"> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">BLO</mi> <mo stretchy="false">(</mo> <mi>ω</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathrm{BLO}(\omega )$</EquationSource> </InlineEquation>, provided that <InlineEquation ID="IEq18"> <EquationSource Format="MATHML"><math> <mi>ω</mi> <mo>∈</mo> <msub> <mi>A</mi> <mn>1</mn> </msub> </math></EquationSource> <EquationSource Format="TEX">$\omega \in A_{1}$</EquationSource> </InlineEquation>. The corresponding John–Nirenberg inequality suitable for the space <InlineEquation ID="IEq19"> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">BLO</mi> <mo stretchy="false">(</mo> <mi>ω</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathrm{BLO}(\omega )$</EquationSource> </InlineEquation> with <InlineEquation ID="IEq20"> <EquationSource Format="MATHML"><math> <mi>ω</mi> <mo>∈</mo> <msub> <mi>A</mi> <mn>1</mn> </msub> </math></EquationSource> <EquationSource Format="TEX">$\omega \in A_{1}$</EquationSource> </InlineEquation> is discussed. Based on this, the equivalent characterization of the space <InlineEquation ID="IEq21"> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">BLO</mi> <mo stretchy="false">(</mo> <mi>ω</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathrm{BLO}(\omega )$</EquationSource> </InlineEquation> is also given.</p>

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Weighted BMO-BLO estimates for Littlewood–Paley square operators

  • Hua Wang,
  • Runzhe Zhang

摘要

Let T ( f ) $T(f)$ denote the Littlewood–Paley square operators, including the Littlewood–Paley G $\mathcal{G}$ -function G ( f ) $\mathcal{G}(f)$ , Lusin’s area integral S ( f ) $\mathcal{S}(f)$ and Stein’s function G λ ( f ) $\mathcal{G}^{\ast}_{\lambda}(f)$ with λ > 2 $\lambda >2$ . We establish the boundedness of Littlewood–Paley square operators on the weighted spaces BMO ( ω ) $\mathrm{BMO}(\omega )$ with ω A 1 $\omega \in A_{1}$ . The weighted space BLO ( ω ) $\mathrm{BLO}(\omega )$ (the space of functions with bounded lower oscillation) is introduced and studied in this paper. This new space is a proper subspace of BMO ( ω ) $\mathrm{BMO}(\omega )$ . It is proved that if T ( f ) ( x 0 ) $T(f)(x_{0})$ is finite for a single point x 0 R n $x_{0}\in \mathbb{R}^{n}$ , then T ( f ) ( x ) $T(f)(x)$ is finite almost everywhere in R n $\mathbb{R}^{n}$ . Moreover, it is shown that T ( f ) $T(f)$ is bounded from BMO ( ω ) $\mathrm{BMO}(\omega )$ into BLO ( ω ) $\mathrm{BLO}(\omega )$ , provided that ω A 1 $\omega \in A_{1}$ . The corresponding John–Nirenberg inequality suitable for the space BLO ( ω ) $\mathrm{BLO}(\omega )$ with ω A 1 $\omega \in A_{1}$ is discussed. Based on this, the equivalent characterization of the space BLO ( ω ) $\mathrm{BLO}(\omega )$ is also given.