<p>Let <i>X</i> be a ball Banach function space on <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2225_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <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>, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2225_Article_IEq2.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(k\in {\mathbb {N}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>k</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2225_Article_IEq3.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="51" /> </InlineMediaObject> <EquationSource Format="TEX">\(h\in {\mathbb {R}}^n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>h</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2225_Article_IEq4.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta ^k_h\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="normal">Δ</mi> <mi>h</mi> <mi>k</mi> </msubsup> </math></EquationSource> </InlineEquation> denote the <i>k</i>-th order difference. In this article, under some mild additional assumptions about <i>X</i>, the authors prove that, for both parameters <i>q</i> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2225_Article_IEq5.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation> in <i>sharp</i> ranges which are related to <i>X</i> and for any locally integrable function <i>f</i> on <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2225_Article_IEq6.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <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> satisfying <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2225_Article_IEq7.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="82" /> </InlineMediaObject> <EquationSource Format="TEX">\(|\nabla ^k f|\in X\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">|</mo> </mrow> <msup> <mi mathvariant="normal">∇</mi> <mi>k</mi> </msup> <mrow> <mi>f</mi> <mo stretchy="false">|</mo> <mo>∈</mo> <mi>X</mi> </mrow> </mrow> </math></EquationSource> </InlineEquation>, <Equation ID="Equ102"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2225_Article_Equ102.gif" Format="GIF" Height="66" Rendition="HTML" Resolution="72" Type="Linedraw" Width="445" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \sup _{\lambda \in (0,\infty )}\lambda \left\| \left[ \int _{\{h\in {\mathbb {R}}^n:\ |\Delta _h^k f(\cdot )|&gt;\lambda |h|^{k+\frac{\gamma }{q}}\}} \left| h\right| ^{\gamma -n}\,dh\right] ^\frac{1}{q}\right\| _X \sim \left\| \,\left| \nabla ^k f\right| \,\right\| _{X} \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <munder> <mo movablelimits="true">sup</mo> <mrow> <mi>λ</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </munder> <mi>λ</mi> <msub> <mfenced close="∥" open="∥"> <msup> <mfenced close="]" open="["> <msub> <mo>∫</mo> <mrow> <mo stretchy="false">{</mo> <mi>h</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo>:</mo> <mspace width="4pt" /> <mo stretchy="false">|</mo> <msubsup> <mi mathvariant="normal">Δ</mi> <mi>h</mi> <mi>k</mi> </msubsup> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">|</mo> <mo>&gt;</mo> <mi>λ</mi> <mo stretchy="false">|</mo> <mi>h</mi> <msup> <mo stretchy="false">|</mo> <mrow> <mi>k</mi> <mo>+</mo> <mfrac> <mi>γ</mi> <mi>q</mi> </mfrac> </mrow> </msup> <mo stretchy="false">}</mo> </mrow> </msub> <msup> <mfenced close="|" open="|"> <mi>h</mi> </mfenced> <mrow> <mi>γ</mi> <mo>-</mo> <mi>n</mi> </mrow> </msup> <mspace width="0.166667em" /> <mi>d</mi> <mi>h</mi> </mfenced> <mfrac> <mn>1</mn> <mi>q</mi> </mfrac> </msup> </mfenced> <mi>X</mi> </msub> <mo>∼</mo> <msub> <mfenced close="∥" open="∥"> <mspace width="0.166667em" /> <mfenced close="|" open="|"> <msup> <mi mathvariant="normal">∇</mi> <mi>k</mi> </msup> <mi>f</mi> </mfenced> <mspace width="0.166667em" /> </mfenced> <mi>X</mi> </msub> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>with the positive equivalence constants independent of <i>f</i>. As applications, the authors establish the Brezis–Seeger–Van Schaftingen–Yung (for short, BSVY) characterization of higher-order homogeneous ball Banach Sobolev spaces and higher-order fractional Gagliardo–Nirenberg and Sobolev type inequalities in critical cases. All these results are of quite wide generality and can be applied to various specific function spaces; moreover, even when <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2225_Article_IEq8.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(X:= L^{q}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>X</mi> <mo>:</mo> <mo>=</mo> <msup> <mi>L</mi> <mi>q</mi> </msup> </mrow> </math></EquationSource> </InlineEquation>, these results when <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2225_Article_IEq9.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(k=1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>k</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> coincide with the best known results and when <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2225_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(k\ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>k</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> are completely new. The first novelty is to establish a sparse characterization of dyadic cubes in level sets related to the higher-order local approximation, which, together with the well-known Whitney inequality in approximation theory, further induces a higher-order weighted variant of the remarkable inequality obtained by A. Cohen, W. Dahmen, I. Daubechies, and R. DeVore; the second novelty is to combine this weighted inequality neatly with a variant higher-order Poincaré inequality to establish the desired upper estimate of BSVY formulae in weighted Lebesgue spaces.</p>

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Sharp Brezis–Seeger–Van Schaftingen–Yung Formulae for Higher-Order Gradients in Ball Banach Function Spaces

  • Pingxu Hu,
  • Yinqin Li,
  • Dachun Yang,
  • Wen Yuan,
  • Yangyang Zhang

摘要

Let X be a ball Banach function space on \({\mathbb {R}}^n\) R n , \(k\in {\mathbb {N}}\) k N , \(h\in {\mathbb {R}}^n\) h R n , and \(\Delta ^k_h\) Δ h k denote the k-th order difference. In this article, under some mild additional assumptions about X, the authors prove that, for both parameters q and \(\gamma \) γ in sharp ranges which are related to X and for any locally integrable function f on \({{\mathbb {R}}^n}\) R n satisfying \(|\nabla ^k f|\in X\) | k f | X , \(\begin{aligned} \sup _{\lambda \in (0,\infty )}\lambda \left\| \left[ \int _{\{h\in {\mathbb {R}}^n:\ |\Delta _h^k f(\cdot )|>\lambda |h|^{k+\frac{\gamma }{q}}\}} \left| h\right| ^{\gamma -n}\,dh\right] ^\frac{1}{q}\right\| _X \sim \left\| \,\left| \nabla ^k f\right| \,\right\| _{X} \end{aligned}\) sup λ ( 0 , ) λ { h R n : | Δ h k f ( · ) | > λ | h | k + γ q } h γ - n d h 1 q X k f X with the positive equivalence constants independent of f. As applications, the authors establish the Brezis–Seeger–Van Schaftingen–Yung (for short, BSVY) characterization of higher-order homogeneous ball Banach Sobolev spaces and higher-order fractional Gagliardo–Nirenberg and Sobolev type inequalities in critical cases. All these results are of quite wide generality and can be applied to various specific function spaces; moreover, even when \(X:= L^{q}\) X : = L q , these results when \(k=1\) k = 1 coincide with the best known results and when \(k\ge 2\) k 2 are completely new. The first novelty is to establish a sparse characterization of dyadic cubes in level sets related to the higher-order local approximation, which, together with the well-known Whitney inequality in approximation theory, further induces a higher-order weighted variant of the remarkable inequality obtained by A. Cohen, W. Dahmen, I. Daubechies, and R. DeVore; the second novelty is to combine this weighted inequality neatly with a variant higher-order Poincaré inequality to establish the desired upper estimate of BSVY formulae in weighted Lebesgue spaces.