<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\cal{X}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mi mathvariant="script">X</mi> </mrow> </math></EquationSource> </InlineEquation> represent either ℝ<sup><i>n</i></sup> or a cube <i>Q</i> of ℝ<sup><i>n</i></sup> with finite edge length. The authors prove that, for any <i>p</i> ∈ (1, ∞), the predual of the dyadic John-Nirenberg space <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(JN_{p}^{{\rm{d}}}({\cal{X}})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mi>p</mi> </mrow> <mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mrow> <mrow> <mi mathvariant="script">X</mi> </mrow> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> is a dyadic Hardy-type space and then establish some relationships among dyadic John-Nirenberg spaces, dyadic Hardy-type spaces, and their non-dyadic counterparts. Moreover, the authors prove that, for any <i>α</i> ∈ [0, <i>n</i>) and <i>p, q</i> ∈ (1, ∞) with <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\({1 \over q} = {1 \over p} - {\alpha \over n}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mfrac> <mn>1</mn> <mi>q</mi> </mfrac> </mrow> <mo>=</mo> <mrow> <mfrac> <mn>1</mn> <mi>p</mi> </mfrac> </mrow> <mo>−</mo> <mrow> <mfrac> <mi>α</mi> <mi>n</mi> </mfrac> </mrow> </math></EquationSource> </InlineEquation>, the fractional dyadic maximal operator <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(M_{{\cal{X}}}^{{\rm{d}},\alpha}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msubsup> <mi>M</mi> <mrow> <mrow> <mrow> <mi mathvariant="script">X</mi> </mrow> </mrow> </mrow> <mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> <mo>,</mo> <mi>α</mi> </mrow> </msubsup> </math></EquationSource> </InlineEquation> is bounded from <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(JN_{p}^{\rm{d}}(\cal{X})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mi>p</mi> </mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> to <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(JN_{q}^{\rm{d}}(\cal{X})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mi>q</mi> </mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> and maps <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(VJN_{p}^{\rm{d}}(\cal{X})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>V</mi> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mi>p</mi> </mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> to <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(VJN_{q}^{\rm{d}}(\cal{X})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>V</mi> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mi>q</mi> </mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(VJN_{p}^{\rm{d}}(\cal{X})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>V</mi> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mi>p</mi> </mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(VJN_{q}^{\rm{d}}(\cal{X})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>V</mi> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mi>q</mi> </mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> are, respectively, the vanishing sub-spaces of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(JN_{p}^{\rm{d}}(\cal{X})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mi>p</mi> </mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(JN_{q}^{\rm{d}}(\cal{X})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mi>q</mi> </mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation>. As for the endpoint case <i>p</i> = 1 and <i>α</i> ∈ (0, <i>n</i>), the authors show <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(M_{\cal{X}}^{{\rm{d,}}\alpha}:JN_1^{\rm{d}}(\cal{X}) \to JN_{{n \over {n - \alpha}}}^{\rm{d}}(\cal{X})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msubsup> <mi>M</mi> <mrow> <mrow> <mi mathvariant="script">X</mi> </mrow> </mrow> <mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> <mo>,</mo> </mrow> </mrow> <mi>α</mi> </mrow> </msubsup> <mo>:</mo> <mi>J</mi> <msubsup> <mi>N</mi> <mn>1</mn> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> <mo stretchy="false">→</mo> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mrow> <mfrac> <mi>n</mi> <mrow> <mi>n</mi> <mo>−</mo> <mi>α</mi> </mrow> </mfrac> </mrow> </mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation>, which improves the classical weak-type result <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(M_{\cal{X}}^{{\rm{d}},\alpha}:{L^1}(\cal{X}) \to {L^{{n \over {n - \alpha}},\infty}}(\cal{X})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msubsup> <mi>M</mi> <mrow> <mrow> <mi mathvariant="script">X</mi> </mrow> </mrow> <mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> <mo>,</mo> <mi>α</mi> </mrow> </msubsup> <mo>:</mo> <mrow> <msup> <mi>L</mi> <mn>1</mn> </msup> </mrow> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> <mo stretchy="false">→</mo> <mrow> <msup> <mi>L</mi> <mrow> <mrow> <mfrac> <mi>n</mi> <mrow> <mi>n</mi> <mo>−</mo> <mi>α</mi> </mrow> </mfrac> </mrow> <mo>,</mo> <mi mathvariant="normal">∞</mi> </mrow> </msup> </mrow> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> because <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(JN_{1}^{\rm{d}}(Q)=L^{1}(Q)\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mn>1</mn> </mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mi>Q</mi> <mo stretchy="false">)</mo> <mo>=</mo> <msup> <mi>L</mi> <mrow> <mn>1</mn> </mrow> </msup> <mo stretchy="false">(</mo> <mi>Q</mi> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> and <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="MediaObjects/11464_2025_214_Fig1_HTML.jpg" Format="JPEG" Height="79" Rendition="HTML" Resolution="300" Type="Linedraw" Width="500" /> </InlineMediaObject>. Compared with recent corresponding results of J. Kinnunen and K. Myyryläinen, both the case <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\cal{X}=\mathbb{R}^{n}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo>=</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mrow> <mi>n</mi> </mrow> </msup> </math></EquationSource> </InlineEquation> and the mapping result on vanishing subspaces are new. Also, an interesting phenomenon in the endpoint case <i>p</i> = 1 is that <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(M_{\cal{X}}^{\rm{d},\alpha}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msubsup> <mi>M</mi> <mrow> <mrow> <mi mathvariant="script">X</mi> </mrow> </mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> <mo>,</mo> <mi>α</mi> </mrow> </msubsup> </math></EquationSource> </InlineEquation> maps <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(JN_{1}^{\rm{d}}(\cal{X})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi>J</mi> <msubsup> <mi>N</mi> <mrow> <mn>1</mn> </mrow> <mrow> <mrow> <mi mathvariant="normal">d</mi> </mrow> </mrow> </msubsup> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="script">X</mi> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> to the convexification of the dyadic John-Nirenberg space when <i>α</i> = 0, but the convexification disappears when <i>α</i> &gt; 0.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Dyadic John-Nirenberg Spaces: Predual Spaces and Fractional Dyadic Maximal Operators

  • Xing Fu,
  • Jin Tao,
  • Dachun Yang

摘要

Let \(\cal{X}\) X represent either ℝn or a cube Q of ℝn with finite edge length. The authors prove that, for any p ∈ (1, ∞), the predual of the dyadic John-Nirenberg space \(JN_{p}^{{\rm{d}}}({\cal{X}})\) J N p d ( X ) is a dyadic Hardy-type space and then establish some relationships among dyadic John-Nirenberg spaces, dyadic Hardy-type spaces, and their non-dyadic counterparts. Moreover, the authors prove that, for any α ∈ [0, n) and p, q ∈ (1, ∞) with \({1 \over q} = {1 \over p} - {\alpha \over n}\) 1 q = 1 p α n , the fractional dyadic maximal operator \(M_{{\cal{X}}}^{{\rm{d}},\alpha}\) M X d , α is bounded from \(JN_{p}^{\rm{d}}(\cal{X})\) J N p d ( X ) to \(JN_{q}^{\rm{d}}(\cal{X})\) J N q d ( X ) and maps \(VJN_{p}^{\rm{d}}(\cal{X})\) V J N p d ( X ) to \(VJN_{q}^{\rm{d}}(\cal{X})\) V J N q d ( X ) , where \(VJN_{p}^{\rm{d}}(\cal{X})\) V J N p d ( X ) and \(VJN_{q}^{\rm{d}}(\cal{X})\) V J N q d ( X ) are, respectively, the vanishing sub-spaces of \(JN_{p}^{\rm{d}}(\cal{X})\) J N p d ( X ) and \(JN_{q}^{\rm{d}}(\cal{X})\) J N q d ( X ) . As for the endpoint case p = 1 and α ∈ (0, n), the authors show \(M_{\cal{X}}^{{\rm{d,}}\alpha}:JN_1^{\rm{d}}(\cal{X}) \to JN_{{n \over {n - \alpha}}}^{\rm{d}}(\cal{X})\) M X d , α : J N 1 d ( X ) J N n n α d ( X ) , which improves the classical weak-type result \(M_{\cal{X}}^{{\rm{d}},\alpha}:{L^1}(\cal{X}) \to {L^{{n \over {n - \alpha}},\infty}}(\cal{X})\) M X d , α : L 1 ( X ) L n n α , ( X ) because \(JN_{1}^{\rm{d}}(Q)=L^{1}(Q)\) J N 1 d ( Q ) = L 1 ( Q ) and . Compared with recent corresponding results of J. Kinnunen and K. Myyryläinen, both the case \(\cal{X}=\mathbb{R}^{n}\) X = R n and the mapping result on vanishing subspaces are new. Also, an interesting phenomenon in the endpoint case p = 1 is that \(M_{\cal{X}}^{\rm{d},\alpha}\) M X d , α maps \(JN_{1}^{\rm{d}}(\cal{X})\) J N 1 d ( X ) to the convexification of the dyadic John-Nirenberg space when α = 0, but the convexification disappears when α > 0.