<p>Given a smooth curve with nonzero curvature <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\Sigma \subset \mathbb {R}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Σ</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation>, let <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(E_{\Sigma }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>E</mi> <mi mathvariant="normal">Σ</mi> </msub> </math></EquationSource> </InlineEquation> denote the associated Fourier extension operator. For both general compact curves and the parabola, we characterize the pairs <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\((p,q)\in [1,\infty ]^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>p</mi> <mo>,</mo> <mi>q</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mrow> <mo stretchy="false">[</mo> <mn>1</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">]</mo> </mrow> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> for which the estimates <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\Vert E_{\Sigma }f\Vert _{L^q(\Omega )}\le C\Vert f\Vert _{L^p(\Sigma )}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">‖</mo> </mrow> <msub> <mi>E</mi> <mi mathvariant="normal">Σ</mi> </msub> <msub> <mrow> <mi>f</mi> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mi>q</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> <mo>≤</mo> <mi>C</mi> <msub> <mrow> <mo stretchy="false">‖</mo> <mi>f</mi> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Σ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\((\mathcal {R}(|E_{\Sigma }f|^{q}))^{\frac{1}{q}}\le C\Vert f\Vert _{L^p(\Sigma )}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">R</mi> <mo stretchy="false">(</mo> <mo stretchy="false">|</mo> </mrow> <msub> <mi>E</mi> <mi mathvariant="normal">Σ</mi> </msub> <msup> <mrow> <mi>f</mi> <mo stretchy="false">|</mo> </mrow> <mi>q</mi> </msup> <msup> <mrow> <mo stretchy="false">)</mo> <mo stretchy="false">)</mo> </mrow> <mfrac> <mn>1</mn> <mi>q</mi> </mfrac> </msup> <mo>≤</mo> <mi>C</mi> <msub> <mrow> <mo stretchy="false">‖</mo> <mi>f</mi> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Σ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> hold, where <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation> is a strip in <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mathbb {R}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\mathcal {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">R</mi> </math></EquationSource> </InlineEquation> denotes the Radon transform. This work continues the study of mass concentration of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(x\mapsto E_{\Sigma }f(x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>↦</mo> <msub> <mi>E</mi> <mi mathvariant="normal">Σ</mi> </msub> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> near lines in <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\mathbb {R}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>, initiated by Bennett and Nakamura [<CitationRef CitationID="CR2">2</CitationRef>] and later extended by Bennett, Nakamura, and the second author in [<CitationRef CitationID="CR3">3</CitationRef>], where expressions of the form <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\((\mathcal {R}(|E_{\Sigma }f|^{2}))^{\frac{1}{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">R</mi> <mo stretchy="false">(</mo> <mo stretchy="false">|</mo> </mrow> <msub> <mi>E</mi> <mi mathvariant="normal">Σ</mi> </msub> <msup> <mrow> <mi>f</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <msup> <mrow> <mo stretchy="false">)</mo> <mo stretchy="false">)</mo> </mrow> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </msup> </mrow> </math></EquationSource> </InlineEquation> were studied.</p>

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Fourier Extension Estimates on a Strip in \(\mathbb {R}^2\)

  • Aleksandar Bulj,
  • Shobu Shiraki

摘要

Given a smooth curve with nonzero curvature \(\Sigma \subset \mathbb {R}^2\) Σ R 2 , let \(E_{\Sigma }\) E Σ denote the associated Fourier extension operator. For both general compact curves and the parabola, we characterize the pairs \((p,q)\in [1,\infty ]^2\) ( p , q ) [ 1 , ] 2 for which the estimates \(\Vert E_{\Sigma }f\Vert _{L^q(\Omega )}\le C\Vert f\Vert _{L^p(\Sigma )}\) E Σ f L q ( Ω ) C f L p ( Σ ) and \((\mathcal {R}(|E_{\Sigma }f|^{q}))^{\frac{1}{q}}\le C\Vert f\Vert _{L^p(\Sigma )}\) ( R ( | E Σ f | q ) ) 1 q C f L p ( Σ ) hold, where \(\Omega \) Ω is a strip in \(\mathbb {R}^2\) R 2 and \(\mathcal {R}\) R denotes the Radon transform. This work continues the study of mass concentration of \(x\mapsto E_{\Sigma }f(x)\) x E Σ f ( x ) near lines in \(\mathbb {R}^2\) R 2 , initiated by Bennett and Nakamura [2] and later extended by Bennett, Nakamura, and the second author in [3], where expressions of the form \((\mathcal {R}(|E_{\Sigma }f|^{2}))^{\frac{1}{2}}\) ( R ( | E Σ f | 2 ) ) 1 2 were studied.