<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation> be a compact patch of a well-curved <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(C^{n+1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>C</mi> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msup> </math></EquationSource> </InlineEquation> curve in <InlineEquation ID="IEq3"> <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> with induced Lebesgue measure <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\textrm{d} \lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>d</mtext> <mi>λ</mi> </mrow> </math></EquationSource> </InlineEquation>, and let <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(g \mapsto \widehat{g \,\textrm{d}\lambda }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>g</mi> <mo>↦</mo> <mover accent="true"> <mrow> <mi>g</mi> <mspace width="0.166667em" /> <mtext>d</mtext> <mi>λ</mi> </mrow> <mo stretchy="true">^</mo> </mover> </mrow> </math></EquationSource> </InlineEquation> be the Fourier extension operator for <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation>. Then we have, for arbitrary non-negative weights <i>w</i>, <Equation ID="Equ82"> <EquationSource Format="TEX">\(\begin{aligned} \int _{B_R} |\widehat{g \,\textrm{d}\lambda }|^2w \le C_{n,a} R^{a} \sup _S \left( \int _S w\right) \int _\Gamma |g|^2 \, \textrm{d} \lambda \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mo>∫</mo> <msub> <mi>B</mi> <mi>R</mi> </msub> </msub> <mrow> <mo stretchy="false">|</mo> </mrow> <mover accent="true"> <mrow> <mi>g</mi> <mspace width="0.166667em" /> <mtext>d</mtext> <mi>λ</mi> </mrow> <mo stretchy="true">^</mo> </mover> <msup> <mrow> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mi>w</mi> <mo>≤</mo> <msub> <mi>C</mi> <mrow> <mi>n</mi> <mo>,</mo> <mi>a</mi> </mrow> </msub> <msup> <mi>R</mi> <mi>a</mi> </msup> <munder> <mo movablelimits="true">sup</mo> <mi>S</mi> </munder> <mfenced close=")" open="("> <msub> <mo>∫</mo> <mi>S</mi> </msub> <mi>w</mi> </mfenced> <msub> <mo>∫</mo> <mi mathvariant="normal">Γ</mi> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>g</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mspace width="0.166667em" /> <mtext>d</mtext> <mi>λ</mi> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>for any <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(a&gt; \frac{n-3}{2} + \frac{2}{n} - \frac{2}{n^2(n+1)}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>&gt;</mo> <mfrac> <mrow> <mi>n</mi> <mo>-</mo> <mn>3</mn> </mrow> <mn>2</mn> </mfrac> <mo>+</mo> <mfrac> <mn>2</mn> <mi>n</mi> </mfrac> <mo>-</mo> <mfrac> <mn>2</mn> <mrow> <msup> <mi>n</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>n</mi> <mo>+</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>, where the <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\sup \)</EquationSource> <EquationSource Format="MATHML"><math> <mo movablelimits="true">sup</mo> </math></EquationSource> </InlineEquation> is over all 1-neighbourhoods <i>S</i> of hyperplanes whose normals are parallel to the tangent at some point of <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation>. This represents partial progress on the Mizohata–Takeuchi conjecture for curves in dimensions <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(n \ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>, improving upon the exponent <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(a=n-1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>=</mo> <mi>n</mi> <mo>-</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> which can be obtained as a consequence of the Agmon–Hörmander trace inequality. Our main tool in establishing this inequality will be a weighted formulation of refined decoupling for well-curved curves. We also discuss the sharpness of the exponents we obtain in this and in auxiliary results, and further explore this in the context of axiomatic decoupling for curves.</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

A Weighted Formulation of Refined Decoupling and Inequalities of Mizohata–Takeuchi-Type for the Moment Curve

  • Anthony Carbery,
  • Zane Kun Li,
  • Yixuan Pang,
  • Po-Lam Yung

摘要

Let \(\Gamma \) Γ be a compact patch of a well-curved \(C^{n+1}\) C n + 1 curve in \(\mathbb {R}^n\) R n with induced Lebesgue measure \(\textrm{d} \lambda \) d λ , and let \(g \mapsto \widehat{g \,\textrm{d}\lambda }\) g g d λ ^ be the Fourier extension operator for \(\Gamma \) Γ . Then we have, for arbitrary non-negative weights w, \(\begin{aligned} \int _{B_R} |\widehat{g \,\textrm{d}\lambda }|^2w \le C_{n,a} R^{a} \sup _S \left( \int _S w\right) \int _\Gamma |g|^2 \, \textrm{d} \lambda \end{aligned}\) B R | g d λ ^ | 2 w C n , a R a sup S S w Γ | g | 2 d λ for any \(a> \frac{n-3}{2} + \frac{2}{n} - \frac{2}{n^2(n+1)}\) a > n - 3 2 + 2 n - 2 n 2 ( n + 1 ) , where the \(\sup \) sup is over all 1-neighbourhoods S of hyperplanes whose normals are parallel to the tangent at some point of \(\Gamma \) Γ . This represents partial progress on the Mizohata–Takeuchi conjecture for curves in dimensions \(n \ge 3\) n 3 , improving upon the exponent \(a=n-1\) a = n - 1 which can be obtained as a consequence of the Agmon–Hörmander trace inequality. Our main tool in establishing this inequality will be a weighted formulation of refined decoupling for well-curved curves. We also discuss the sharpness of the exponents we obtain in this and in auxiliary results, and further explore this in the context of axiomatic decoupling for curves.