Decay of the radius of spatial analyticity for the modified KdV equation and the nonlinear Schrödinger equation with third order dispersion

Renata O. Figueira, Mahendra Panthee
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Abstract

We consider the initial value problems (IVPs) for the modified Korteweg–de Vries (mKdV) equation

$$\begin{aligned} \left\{ \begin{array}{l} \partial _t u+ \partial _x^3u+\mu u^2\partial _xu =0, \quad x\in \mathbb {R},\; t\in \mathbb {R}, \\ u(x,0) = u_0(x), \end{array}\right. \end{aligned}$$

where u is a real valued function and \(\mu =\pm 1\), and the cubic nonlinear Schrödinger equation with third order dispersion (tNLS equation in short)

$$\begin{aligned} \left\{ \begin{array}{l} \partial _t v+i\alpha \partial _x^2v+\beta \partial _x^3v+i\gamma |v|^2v = 0, \quad x\in \mathbb {R},\; t\in \mathbb {R}, \\ v(x,0) = v_0(x), \end{array}\right. \end{aligned}$$

where \(\alpha , \beta \) and \(\gamma \) are real constants and v is a complex valued function. In both problems, the initial data \(u_0\) and \(v_0\) are analytic on \(\mathbb {R}\) and have uniform radius of analyticity \(\sigma _0\) in the space variable. We prove that the both IVPs are locally well-posed for such data by establishing an analytic version of the trilinear estimates, and showed that the radius of spatial analyticity of the solution remains the same \(\sigma _0\) till some lifespan \(0<T_0\le 1\). We also consider the evolution of the radius of spatial analyticity \(\sigma (t)\) when the local solution extends globally in time and prove that for any time \(T\ge T_0\) it is bounded from below by \(c T^{-\frac{4}{3}}\), for the mKdV equation in the defocusing case (\(\mu = -1\)) and by \(c T^{-(4+\varepsilon )}\), \(\varepsilon >0\), for the tNLS equation. The result for the mKdV equation improves the one obtained in Bona et al. (Ann Inst Henri Poincaré 22:783–797, 2005) and, as far as we know, the result for the tNLS equation is the new one.

修正 KdV 方程和三阶分散非线性薛定谔方程空间解析性半径的衰减
我们考虑修正的 Korteweg-de Vries(mKdV)方程的初值问题(IVPs) $$\begin{aligned}\left\{ \begin{array}{l}\partial _t u+partial _x^3u+mu u^2partial _xu =0, quad x in \mathbb {R},\; t in \mathbb {R}, \ u(x,0) = u_0(x), end{array}\right.\end{aligned}$$where u is a real valued function and \(\mu =\pm 1\), and the cubic nonlinear Schrödinger equation with third order dispersion (tNLS equation in short) $$\begin{aligned}.\left\{ \begin{array}{l}\partial _t v+i\alpha \partial _x^2v+i\beta \partial _x^3v+i\gamma |v|^2v = 0, \quad x\in \mathbb {R},\; t\in \mathbb {R}, \v(x,0) = v_0(x), \end{array}\right.\end{aligned}$ 其中 \(\alpha , \beta \) 和 \(\gamma \) 是实常数,v 是复值函数。在这两个问题中,初始数据 \(u_0\) 和 \(v_0\) 在 \(\mathbb {R}\) 上是解析的,并且在空间变量中具有均匀的解析半径 \(\sigma _0\) 。我们通过建立三线性估计的解析版本来证明这两个IVP对这样的数据都是局部良好求解的,并证明解的空间解析半径在某个生命期\(0<T_0\le 1\)之前保持不变\(\sigma _0\)。我们还考虑了当局部解在时间上全局扩展时空间解析性半径的演化,并证明对于任意时间\(T\ge T_0\),空间解析性半径从下往上受\(c T^{-\frac{4}{3}}\) 约束、(\(\mu=-1/)),对于失焦情况下的mKdV方程,由\(c T^{-(4+\varepsilon )}\), (\(\varepsilon >;0),用于 tNLS 方程。mKdV 方程的结果改进了博纳等人(Ann Inst Henri Poincaré 22:783-797, 2005)的结果,据我们所知,tNLS 方程的结果是新的结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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