<p>We establish that the Fourier transform <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathscr {F}: L^p({\mathbb {R}^d})\rightarrow L^{p',p}({\mathbb {R}^d})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">F</mi> <mo>:</mo> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">→</mo> <msup> <mi>L</mi> <mrow> <msup> <mi>p</mi> <mo>′</mo> </msup> <mo>,</mo> <mi>p</mi> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, for <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(d\in {\mathbb {N}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(1&lt;p&lt;2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, is not strictly singular, thereby confirming the optimality of the source and target spaces. A&#xa0;similar result is obtained for Fourier series on <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(L^p(\mathbb {T}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">T</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, with sequence Lorentz spaces as the target. These findings complement known results, which state that <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathscr {F}: L^p({\mathbb {R}^d})\rightarrow L^{p'}({\mathbb {R}^d})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">F</mi> <mo>:</mo> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">→</mo> <msup> <mi>L</mi> <msup> <mi>p</mi> <mo>′</mo> </msup> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is finitely strictly singular and then also strictly singular, and provide further insight into the degrees of non-compactness of&#xa0;<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mathscr {F}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">F</mi> </math></EquationSource> </InlineEquation>.</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

Quantitative Non-Compactness Properties of the Fourier Transform on Optimal Spaces

  • David E. Edmunds,
  • Petr Gurka,
  • Jan Lang

摘要

We establish that the Fourier transform \(\mathscr {F}: L^p({\mathbb {R}^d})\rightarrow L^{p',p}({\mathbb {R}^d})\) F : L p ( R d ) L p , p ( R d ) , for \(d\in {\mathbb {N}}\) d N and \(1<p<2\) 1 < p < 2 , is not strictly singular, thereby confirming the optimality of the source and target spaces. A similar result is obtained for Fourier series on \(L^p(\mathbb {T}^n)\) L p ( T n ) , with sequence Lorentz spaces as the target. These findings complement known results, which state that \(\mathscr {F}: L^p({\mathbb {R}^d})\rightarrow L^{p'}({\mathbb {R}^d})\) F : L p ( R d ) L p ( R d ) is finitely strictly singular and then also strictly singular, and provide further insight into the degrees of non-compactness of  \(\mathscr {F}\) F .