<p>In this paper we prove a higher dimensional analogue of Carleson’s <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi>ε</mi> <mn>2</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">$\varepsilon ^{2}$</EquationSource> </InlineEquation> conjecture. Given two arbitrary disjoint Borel sets <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="107" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi mathvariant="normal">Ω</mi> <mo>+</mo> </msup> <mo>,</mo> <msup> <mi mathvariant="normal">Ω</mi> <mo>−</mo> </msup> <mo>⊂</mo> <msup> <mi mathvariant="double-struck">R</mi> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> </math></EquationSource> <EquationSource Format="TEX">$\Omega ^{+},\Omega ^{-}\subset \mathbb{R}^{n+1}$</EquationSource> </InlineEquation>, and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq5.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="65" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>x</mi> <mo>∈</mo> <msup> <mi mathvariant="double-struck">R</mi> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> </math></EquationSource> <EquationSource Format="TEX">$x\in \mathbb{R}^{n+1}$</EquationSource> </InlineEquation>, <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq6.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>r</mi> <mo>&gt;</mo> <mn>0</mn> </math></EquationSource> <EquationSource Format="TEX">$r&gt;0$</EquationSource> </InlineEquation>, we denote <Equation ID="Equa"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_Equa.gif" Format="GIF" Height="37" Rendition="HTML" Resolution="72" Type="Linedraw" Width="528" /> </MediaObject> <EquationSource Format="MATHML"><math> <msub> <mi>ε</mi> <mi>n</mi> </msub> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>r</mi> <mo stretchy="false">)</mo> <mo>:</mo> <mo>=</mo> <mfrac> <mn>1</mn> <msup> <mi>r</mi> <mi>n</mi> </msup> </mfrac> <mspace width="0.2em" /> <munder> <mo movablelimits="false">inf</mo> <msup> <mi>H</mi> <mo>+</mo> </msup> </munder> <msup> <mi mathvariant="script">H</mi> <mi>n</mi> </msup> <mrow> <mo>(</mo> <mo stretchy="false">(</mo> <mo stretchy="false">(</mo> <mi>∂</mi> <mi>B</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>r</mi> <mo stretchy="false">)</mo> <mo>∩</mo> <msup> <mi>H</mi> <mo>+</mo> </msup> <mo stretchy="false">)</mo> <mo>∖</mo> <msup> <mi mathvariant="normal">Ω</mi> <mo>+</mo> </msup> <mo stretchy="false">)</mo> <mo>∪</mo> <mo stretchy="false">(</mo> <mo stretchy="false">(</mo> <mi>∂</mi> <mi>B</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>r</mi> <mo stretchy="false">)</mo> <mo>∩</mo> <msup> <mi>H</mi> <mo>−</mo> </msup> <mo stretchy="false">)</mo> <mo>∖</mo> <msup> <mi mathvariant="normal">Ω</mi> <mo>−</mo> </msup> <mo stretchy="false">)</mo> <mo>)</mo> </mrow> <mo>,</mo> </math></EquationSource> <EquationSource Format="TEX">\( \varepsilon _{n}(x,r) := \frac{1}{r^{n}}\, \inf _{H^{+}} \mathcal{H}^{n} \left ( ((\partial B(x,r)\cap H^{+}) \setminus \Omega ^{+}) \cup (( \partial B(x,r)\cap H^{-}) \setminus \Omega ^{-})\right ), \)</EquationSource> </Equation> where the infimum is taken over all open affine half-spaces <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi>H</mi> <mo>+</mo> </msup> </math></EquationSource> <EquationSource Format="TEX">$H^{+}$</EquationSource> </InlineEquation> such that <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq8.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>x</mi> <mo>∈</mo> <mi>∂</mi> <msup> <mi>H</mi> <mo>+</mo> </msup> </math></EquationSource> <EquationSource Format="TEX">$x \in \partial H^{+}$</EquationSource> </InlineEquation> and we define <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq9.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="123" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi>H</mi> <mo>−</mo> </msup> <mo>=</mo> <msup> <mi mathvariant="double-struck">R</mi> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> <mo>∖</mo> <mover accent="true"> <msup> <mi>H</mi> <mo>+</mo> </msup> <mo>‾</mo> </mover> </math></EquationSource> <EquationSource Format="TEX">$H^{-}= \mathbb{R}^{n+1} \setminus \overline{H^{+}}$</EquationSource> </InlineEquation>. Our first main result asserts that the set of points <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq5.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="65" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>x</mi> <mo>∈</mo> <msup> <mi mathvariant="double-struck">R</mi> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> </math></EquationSource> <EquationSource Format="TEX">$x\in \mathbb{R}^{n+1}$</EquationSource> </InlineEquation> where <Equation ID="Equb"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_Equb.gif" Format="GIF" Height="44" Rendition="HTML" Resolution="72" Type="Linedraw" Width="151" /> </MediaObject> <EquationSource Format="MATHML"><math> <msubsup> <mo>∫</mo> <mrow> <mn>0</mn> </mrow> <mn>1</mn> </msubsup> <msub> <mi>ε</mi> <mi>n</mi> </msub> <msup> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>r</mi> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </msup> <mspace width="0.2em" /> <mfrac> <mrow> <mi>d</mi> <mi>r</mi> </mrow> <mi>r</mi> </mfrac> <mo>&lt;</mo> <mi mathvariant="normal">∞</mi> </math></EquationSource> <EquationSource Format="TEX">\( \int _{0}^{1} \varepsilon _{n}(x,r)^{2} \, \frac{dr}{r}&lt; \infty \)</EquationSource> </Equation> is <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq11.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>n</mi> </math></EquationSource> <EquationSource Format="TEX">$n$</EquationSource> </InlineEquation>-rectifiable. For our second main result we assume that <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq12.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi mathvariant="normal">Ω</mi> <mo>+</mo> </msup> </math></EquationSource> <EquationSource Format="TEX">$\Omega ^{+}$</EquationSource> </InlineEquation>, <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq13.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi mathvariant="normal">Ω</mi> <mo>−</mo> </msup> </math></EquationSource> <EquationSource Format="TEX">$\Omega ^{-}$</EquationSource> </InlineEquation> are open and that <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq14.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="64" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi mathvariant="normal">Ω</mi> <mo>+</mo> </msup> <mo>∪</mo> <msup> <mi mathvariant="normal">Ω</mi> <mo>−</mo> </msup> </math></EquationSource> <EquationSource Format="TEX">$\Omega ^{+}\cup \Omega ^{-}$</EquationSource> </InlineEquation> satisfies the capacity density condition. For each <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq15.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="115" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>x</mi> <mo>∈</mo> <mi>∂</mi> <msup> <mi mathvariant="normal">Ω</mi> <mo>+</mo> </msup> <mo>∪</mo> <mi>∂</mi> <msup> <mi mathvariant="normal">Ω</mi> <mo>−</mo> </msup> </math></EquationSource> <EquationSource Format="TEX">$x \in \partial \Omega ^{+} \cup \partial \Omega ^{-}$</EquationSource> </InlineEquation> and <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq6.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>r</mi> <mo>&gt;</mo> <mn>0</mn> </math></EquationSource> <EquationSource Format="TEX">$r&gt;0$</EquationSource> </InlineEquation>, we denote by <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq17.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi>α</mi> <mo>±</mo> </msup> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>r</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\alpha ^{\pm }(x,r)$</EquationSource> </InlineEquation> the characteristic constant of the (spherical) open sets <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq18.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="103" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi mathvariant="normal">Ω</mi> <mo>±</mo> </msup> <mo>∩</mo> <mi>∂</mi> <mi>B</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>r</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\Omega ^{\pm }\cap \partial B(x,r)$</EquationSource> </InlineEquation>. We show that, up to a set of <InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq19.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="25" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi mathvariant="script">H</mi> <mi>n</mi> </msup> </math></EquationSource> <EquationSource Format="TEX">$\mathcal{H}^{n}$</EquationSource> </InlineEquation> measure zero, <InlineEquation ID="IEq20"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq20.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>x</mi> </math></EquationSource> <EquationSource Format="TEX">$x$</EquationSource> </InlineEquation> is a tangent point for both <InlineEquation ID="IEq21"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq21.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>∂</mi> <msup> <mi mathvariant="normal">Ω</mi> <mo>+</mo> </msup> </math></EquationSource> <EquationSource Format="TEX">$\partial \Omega ^{+}$</EquationSource> </InlineEquation> and <InlineEquation ID="IEq22"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq22.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>∂</mi> <msup> <mi mathvariant="normal">Ω</mi> <mo>−</mo> </msup> </math></EquationSource> <EquationSource Format="TEX">$\partial \Omega ^{-}$</EquationSource> </InlineEquation> if and only if <Equation ID="Equc"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_Equc.gif" Format="GIF" Height="44" Rendition="HTML" Resolution="72" Type="Linedraw" Width="311" /> </MediaObject> <EquationSource Format="MATHML"><math> <msubsup> <mo>∫</mo> <mrow> <mn>0</mn> </mrow> <mn>1</mn> </msubsup> <mo movablelimits="false">min</mo> <mo stretchy="false">(</mo> <mn>1</mn> <mo>,</mo> <msup> <mi>α</mi> <mo>+</mo> </msup> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>r</mi> <mo stretchy="false">)</mo> <mo>+</mo> <msup> <mi>α</mi> <mo>−</mo> </msup> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>r</mi> <mo stretchy="false">)</mo> <mo>−</mo> <mn>2</mn> <mo stretchy="false">)</mo> <mfrac> <mrow> <mi>d</mi> <mi>r</mi> </mrow> <mi>r</mi> </mfrac> <mo>&lt;</mo> <mi mathvariant="normal">∞</mi> <mo>.</mo> </math></EquationSource> <EquationSource Format="TEX">\( \int _{0}^{1} \min (1,\alpha ^{+}(x,r) + \alpha ^{-}(x,r) -2) \frac{dr}{r} &lt; \infty . \)</EquationSource> </Equation> The first result is new even in the plane and the second one improves and extends to higher dimensions the <InlineEquation ID="IEq23"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="222_2025_1337_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi>ε</mi> <mn>2</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">$\varepsilon ^{2}$</EquationSource> </InlineEquation> conjecture of Carleson.</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

Carleson’s \(\varepsilon ^{2}\) conjecture in higher dimensions

  • Ian Fleschler,
  • Xavier Tolsa,
  • Michele Villa

摘要

In this paper we prove a higher dimensional analogue of Carleson’s ε 2 $\varepsilon ^{2}$ conjecture. Given two arbitrary disjoint Borel sets Ω + , Ω R n + 1 $\Omega ^{+},\Omega ^{-}\subset \mathbb{R}^{n+1}$ , and x R n + 1 $x\in \mathbb{R}^{n+1}$ , r > 0 $r>0$ , we denote ε n ( x , r ) : = 1 r n inf H + H n ( ( ( B ( x , r ) H + ) Ω + ) ( ( B ( x , r ) H ) Ω ) ) , \( \varepsilon _{n}(x,r) := \frac{1}{r^{n}}\, \inf _{H^{+}} \mathcal{H}^{n} \left ( ((\partial B(x,r)\cap H^{+}) \setminus \Omega ^{+}) \cup (( \partial B(x,r)\cap H^{-}) \setminus \Omega ^{-})\right ), \) where the infimum is taken over all open affine half-spaces H + $H^{+}$ such that x H + $x \in \partial H^{+}$ and we define H = R n + 1 H + $H^{-}= \mathbb{R}^{n+1} \setminus \overline{H^{+}}$ . Our first main result asserts that the set of points x R n + 1 $x\in \mathbb{R}^{n+1}$ where 0 1 ε n ( x , r ) 2 d r r < \( \int _{0}^{1} \varepsilon _{n}(x,r)^{2} \, \frac{dr}{r}< \infty \) is n $n$ -rectifiable. For our second main result we assume that Ω + $\Omega ^{+}$ , Ω $\Omega ^{-}$ are open and that Ω + Ω $\Omega ^{+}\cup \Omega ^{-}$ satisfies the capacity density condition. For each x Ω + Ω $x \in \partial \Omega ^{+} \cup \partial \Omega ^{-}$ and r > 0 $r>0$ , we denote by α ± ( x , r ) $\alpha ^{\pm }(x,r)$ the characteristic constant of the (spherical) open sets Ω ± B ( x , r ) $\Omega ^{\pm }\cap \partial B(x,r)$ . We show that, up to a set of H n $\mathcal{H}^{n}$ measure zero, x $x$ is a tangent point for both Ω + $\partial \Omega ^{+}$ and Ω $\partial \Omega ^{-}$ if and only if 0 1 min ( 1 , α + ( x , r ) + α ( x , r ) 2 ) d r r < . \( \int _{0}^{1} \min (1,\alpha ^{+}(x,r) + \alpha ^{-}(x,r) -2) \frac{dr}{r} < \infty . \) The first result is new even in the plane and the second one improves and extends to higher dimensions the ε 2 $\varepsilon ^{2}$ conjecture of Carleson.