<p>In this paper, we consider a rough Fourier integral operator defined as <Equation ID="Equ9"> <EquationSource Format="TEX">\(T_{\phi ,a}f(x)=\int \limits _{\mathbb {R}^{n}}e^{i\phi (x,\xi )}a(x,\xi )\hat{f}(\xi )d\xi ,\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <msub> <mi>T</mi> <mrow> <mi>ϕ</mi> <mo>,</mo> <mi>a</mi> </mrow> </msub> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <munder> <mo movablelimits="false">∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </munder> <msup> <mi>e</mi> <mrow> <mi>i</mi> <mi>ϕ</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>ξ</mi> <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="false">^</mo> </mover> <mrow> <mo stretchy="false">(</mo> <mi>ξ</mi> <mo stretchy="false">)</mo> </mrow> <mi>d</mi> <mi>ξ</mi> <mo>,</mo> </mrow> </math></EquationSource> </Equation>where the amplitude <InlineEquation ID="IEq4"> <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 the phase <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\phi \in L^{\infty }\Phi ^{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϕ</mi> <mo>∈</mo> <msup> <mi>L</mi> <mi>∞</mi> </msup> <msup> <mi mathvariant="normal">Φ</mi> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> satisfy the rough <i>k</i>-corank condition. The motivation for this problem stems from the regularity of the maximal wave operator. We prove that this operator is bounded from <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(L^{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation> to <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(L_{\text {loc}}^{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>L</mi> <mrow> <mtext>loc</mtext> </mrow> <mn>2</mn> </msubsup> </math></EquationSource> </InlineEquation> provided <Equation ID="Equ10"> <EquationSource Format="TEX">\(m&lt;\min \left\{ \frac{n(\rho -1)}{2},\frac{\rho }{2}-\frac{n+1}{4}\right\} -\frac{k\rho }{2}.\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mi>m</mi> <mo>&lt;</mo> <mo movablelimits="true">min</mo> <mfenced close="}" open="{"> <mfrac> <mrow> <mi>n</mi> <mo stretchy="false">(</mo> <mi>ρ</mi> <mo>-</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </mfrac> <mo>,</mo> <mfrac> <mi>ρ</mi> <mn>2</mn> </mfrac> <mo>-</mo> <mfrac> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> <mn>4</mn> </mfrac> </mfenced> <mo>-</mo> <mfrac> <mrow> <mi>k</mi> <mi>ρ</mi> </mrow> <mn>2</mn> </mfrac> <mo>.</mo> </mrow> </math></EquationSource> </Equation></p>

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Local \(L^2\)-boundedness of rough Fourier integral operators with the rough corank condition

  • Xiao Yu,
  • Xiangrong Zhu

摘要

In this paper, we consider a rough Fourier integral operator defined as \(T_{\phi ,a}f(x)=\int \limits _{\mathbb {R}^{n}}e^{i\phi (x,\xi )}a(x,\xi )\hat{f}(\xi )d\xi ,\) T ϕ , a f ( x ) = R n e i ϕ ( 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 the phase \(\phi \in L^{\infty }\Phi ^{2}\) ϕ L Φ 2 satisfy the rough k-corank condition. The motivation for this problem stems from the regularity of the maximal wave operator. We prove that this operator is bounded from \(L^{2}\) L 2 to \(L_{\text {loc}}^{2}\) L loc 2 provided \(m<\min \left\{ \frac{n(\rho -1)}{2},\frac{\rho }{2}-\frac{n+1}{4}\right\} -\frac{k\rho }{2}.\) m < min n ( ρ - 1 ) 2 , ρ 2 - n + 1 4 - k ρ 2 .