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arXiv 2103.10718math.AP
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Gross-Pitaevskii方程的相互作用螺旋行波解

Interacting helical traveling waves for the Gross-Pitaevskii equation

Juan Dávila, Manuel del Pino, María Medina, Rémy Rodiac

摘要:

我们考虑3D Gross-Pitaevskii方程\begin{equation}\nonumber i\partial_t ψ+Δψ+(1-|ψ|^2)ψ=0 \text{ for } ψ:\mathbb{R}\times \mathbb{R}^3 \rightarrow \mathbb{C} \end{equation}并构造该方程的行波解。这些解的形式为$ψ(t,x)=u(x_1,x_2,x_3-Ct)$,速度$C$的阶数为$\varepsilon|\log\varepsilon|$,参数为小参数$\varepsilon>0$。我们构建两种不同类型的解决方案。对于第一种类型,函数$u$具有接近于$n\geq 2$的$n$螺旋的并集的零集(涡集),并且在这些螺旋附近$u$具有1度。对于第二种类型,函数$u$在垂直轴$e_3$附近具有度为$-1$的涡丝,在轴为$e_3$的螺旋附近具有度为$+1$的$n\geq 4$涡丝。在这两种情况下,螺旋线的距离为$1/(\varepsilon\sqrt{|\log \varepsilon|)}$级,是克莱因-马格达-达摩达兰系统的解,该系统用来描述理想流体中几乎平行的涡丝的演化。最近,作者对定常的Gross-Pitaevskii方程,即Ginzburg-Landau方程构造了类似的解。为了证明这些解决方案的存在性,我们使用Lyapunov-Schmidt方法和一个微妙的偶数和奇数傅立叶模式之间的误差的一个适当的近似分离。

英文摘要:

We consider the 3D Gross-Pitaevskii equation \begin{equation}\nonumber i\partial_t ψ+Δψ+(1-|ψ|^2)ψ=0 \text{ for } ψ:\mathbb{R}\times \mathbb{R}^3 \rightarrow \mathbb{C} \end{equation} and construct traveling waves solutions to this equation. These are solutions of the form $ψ(t,x)=u(x_1,x_2,x_3-Ct)$ with a velocity $C$ of order $\varepsilon|\log\varepsilon|$ for a small parameter $\varepsilon>0$. We build two different types of solutions. For the first type, the functions $u$ have a zero-set (vortex set) close to an union of $n$ helices for $n\geq 2$ and near these helices $u$ has degree 1. For the second type, the functions $u$ have a vortex filament of degree $-1$ near the vertical axis $e_3$ and $n\geq 4$ vortex filaments of degree $+1$ near helices whose axis is $e_3$. In both cases the helices are at a distance of order $1/(\varepsilon\sqrt{|\log \varepsilon|)}$ from the axis and are solutions to the Klein-Majda-Damodaran system, supposed to describe the evolution of nearly parallel vortex filaments in ideal fluids. Analogous solutions have been constructed recently by the authors for the stationary Gross-Pitaevskii equation, namely the Ginzburg-Landau equation. To prove the existence of these solutions we use the Lyapunov-Schmidt method and a subtle separation between even and odd Fourier modes of the error of a suitable approximation.

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