<p>In this paper, consideration is given to the initial value problem associated with the higher-dimensional fourth-order nonlinear Schrödinger equations <Equation ID="Equ34"> <EquationSource Format="TEX">\(\begin{aligned} i\partial _tu-\Delta ^2u =|u |^2u, \qquad (x, t)\in \mathbb {R}^d\times \mathbb {R} \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mi>i</mi> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mi>u</mi> <mo>-</mo> <msup> <mi mathvariant="normal">Δ</mi> <mn>2</mn> </msup> <mi>u</mi> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mi>u</mi> <mo>,</mo> <mspace width="2em" /> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> <mo>×</mo> <mi mathvariant="double-struck">R</mi> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>with initial data <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(u_0(x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>u</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> in the modified Gevrey spaces <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(H^{\sigma ,2}(\mathbb {R}^d)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>H</mi> <mrow> <mi>σ</mi> <mo>,</mo> <mn>2</mn> </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="IEq5"> <EquationSource Format="TEX">\(d=2,3,4\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>=</mo> <mn>2</mn> <mo>,</mo> <mn>3</mn> <mo>,</mo> <mn>4</mn> </mrow> </math></EquationSource> </InlineEquation>. We show that the uniform radius of spatial analyticity <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\sigma (t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>σ</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> of solution at time <i>t</i> does not decay faster than <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(|t|^{-\frac{1}{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mo stretchy="false">|</mo> <mi>t</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </mrow> </msup> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(|t| \rightarrow \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">|</mo> <mi>t</mi> <mo stretchy="false">|</mo> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. Our proof relies on approximate conservation law in modified Gevrey spaces, space-time estimates and Sobolev embedding.</p>

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Asymptotic lower bounds on the spatial analyticity radius for solutions to the fourth-order nonlinear Schrödinger equation on \(\mathbb {R}^d\)

  • Betre Shiferaw,
  • Tegegne Getachew

摘要

In this paper, consideration is given to the initial value problem associated with the higher-dimensional fourth-order nonlinear Schrödinger equations \(\begin{aligned} i\partial _tu-\Delta ^2u =|u |^2u, \qquad (x, t)\in \mathbb {R}^d\times \mathbb {R} \end{aligned}\) i t u - Δ 2 u = | u | 2 u , ( x , t ) R d × R with initial data \(u_0(x)\) u 0 ( x ) in the modified Gevrey spaces \(H^{\sigma ,2}(\mathbb {R}^d)\) H σ , 2 ( R d ) for \(d=2,3,4\) d = 2 , 3 , 4 . We show that the uniform radius of spatial analyticity \(\sigma (t)\) σ ( t ) of solution at time t does not decay faster than \(|t|^{-\frac{1}{2}}\) | t | - 1 2 as \(|t| \rightarrow \infty \) | t | . Our proof relies on approximate conservation law in modified Gevrey spaces, space-time estimates and Sobolev embedding.