<p>In this note, we consider a general maximal wave operator defined by <Equation ID="Equ15"> <EquationSource Format="TEX">\(\begin{aligned} W_{a,t}f(x)=\int _{\mathbb {R}^{n}}e^{i(x\cdot \xi +t(x)|\xi |)}a(x,\xi )\widehat{f}(\xi )d\xi , \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>W</mi> <mrow> <mi>a</mi> <mo>,</mo> <mi>t</mi> </mrow> </msub> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </msub> <msup> <mi>e</mi> <mrow> <mi>i</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>·</mo> <mi>ξ</mi> <mo>+</mo> <mi>t</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mo stretchy="false">|</mo> <mi>ξ</mi> <mo stretchy="false">|</mo> <mo stretchy="false">)</mo> </mrow> </msup> <mi>a</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>ξ</mi> <mo stretchy="false">)</mo> </mrow> <mover accent="true"> <mi>f</mi> <mo stretchy="true">^</mo> </mover> <mrow> <mo stretchy="false">(</mo> <mi>ξ</mi> <mo stretchy="false">)</mo> </mrow> <mi>d</mi> <mi>ξ</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where the amplitude <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(a\in L^{\infty }S^{m}_{\rho }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>∈</mo> <msup> <mi>L</mi> <mi>∞</mi> </msup> <msubsup> <mi>S</mi> <mi>ρ</mi> <mi>m</mi> </msubsup> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(t\in L^{\infty }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>∈</mo> <msup> <mi>L</mi> <mi>∞</mi> </msup> </mrow> </math></EquationSource> </InlineEquation>. We prove that this operator is bounded on <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(L^{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation> provided <Equation ID="Equ16"> <EquationSource Format="TEX">\(\begin{aligned} m&lt;\frac{(n-1)\rho -n}{2}. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mi>m</mi> <mo>&lt;</mo> <mfrac> <mrow> <mo stretchy="false">(</mo> <mi>n</mi> <mo>-</mo> <mn>1</mn> <mo stretchy="false">)</mo> <mi>ρ</mi> <mo>-</mo> <mi>n</mi> </mrow> <mn>2</mn> </mfrac> <mo>.</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>As a direct application, we obtain the well-known result that the maximal wave operator <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(W^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>W</mi> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation> is bounded from the Sobolev space <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(H^s=W^{s,2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>H</mi> <mi>s</mi> </msup> <mo>=</mo> <msup> <mi>W</mi> <mrow> <mi>s</mi> <mo>,</mo> <mn>2</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> to <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(L^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation> if <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(s&gt;\frac{1}{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>&gt;</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. This result is known to be sharp for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(s&gt;\frac{1}{2}.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>&gt;</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Regularities of General Maximal Wave Operators

  • Shoufeng Shen,
  • Xiangrong Zhu

摘要

In this note, we consider a general maximal wave operator defined by \(\begin{aligned} W_{a,t}f(x)=\int _{\mathbb {R}^{n}}e^{i(x\cdot \xi +t(x)|\xi |)}a(x,\xi )\widehat{f}(\xi )d\xi , \end{aligned}\) W a , t f ( x ) = R n e i ( x · ξ + t ( x ) | ξ | ) a ( x , ξ ) f ^ ( ξ ) d ξ , where the amplitude \(a\in L^{\infty }S^{m}_{\rho }\) a L S ρ m and \(t\in L^{\infty }\) t L . We prove that this operator is bounded on \(L^{2}\) L 2 provided \(\begin{aligned} m<\frac{(n-1)\rho -n}{2}. \end{aligned}\) m < ( n - 1 ) ρ - n 2 . As a direct application, we obtain the well-known result that the maximal wave operator \(W^*\) W is bounded from the Sobolev space \(H^s=W^{s,2}\) H s = W s , 2 to \(L^2\) L 2 if \(s>\frac{1}{2}\) s > 1 2 . This result is known to be sharp for \(s>\frac{1}{2}.\) s > 1 2 . .