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Long-time asymptotics for the focusing nonlinear Schr'odinger equation with nonzero boundary conditions at infinity and asymptotic stage of modulational instability

机译:聚焦非线性schr \“odinger方程的长期渐近性   具有非零边界条件的无穷远和渐近阶段   调制不稳定性

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摘要

The long-time asymptotic behavior of the focusing nonlinear Schr\"odinger(NLS) equation on the line with symmetric nonzero boundary conditions atinfinity is characterized by using the recently developed inverse scatteringtransform (IST) for such problems and by employing the nonlinear steepestdescent method of Deift and Zhou for oscillatory Riemann-Hilbert problems.First, the IST is formulated over a single sheet of the complex plane withoutintroducing a uniformization variable. The solution of the focusing NLSequation with nonzero boundary conditions is thus associated with a suitablematrix Riemann-Hilbert problem whose jumps grow exponentially with time forcertain portions of the continuous spectrum. This growth is the signature ofthe well-known modulational instability within the context of the IST. Thisgrowth is then removed by suitable deformations of the Riemann-Hilbert problemin the complex spectral plane. Asymptotically in time, the $xt$-plane is foundto decompose into two types of regions: a left far-field region and a rightfar-field region, where the solution equals the condition at infinity toleading order up to a phase shift, and a central region in which the asymptoticbehavior is described by slowly modulated periodic oscillations. In the latterregion, it is also shown that the modulus of the leading order solution, whichis initially obtained in the form of a ratio of Jacobi theta functions,eventually reduces to the well-known elliptic solution of the focusing NLSequation. These results provide the first characterization of the long-timebehavior of generic perturbations of a constant background in a modulationallyunstable medium.
机译:具有无限对称对称非零边界条件的直线上的聚焦非线性Schr \“ odinger(NLS)方程的长期渐近行为的特征是,针对此类问题,使用了最近开发的逆散射变换(IST),并采用了非线性的陡峭下降方法。首先,在不引入均匀化变量的情况下,在单个平面的复杂平面上制定IST,因此将具有非零边界条件的聚焦NLS方程的解与合适的矩阵Riemann-Hilbert问题相关联在连续光谱的某些部分中,跳跃随时间呈指数增长,这种增长是IST内众所周知的调制不稳定性的特征,然后通过复杂光谱平面中黎曼-希尔伯特问题的适当变形消除了这种增长。时间,发现$ xt $平面分解为两种类型s个区域:左远场区域和右远场区域,其中解等于无穷大的条件,直至导致相移的前导阶数;中心区域,通过渐进调制的周期性振荡描述渐近行为。在后一个区域中,还显示出,最初以Jacobi theta函数的比率形式获得的前导解的模量最终减小为聚焦NLS方程的椭圆形解。这些结果首次表征了调制不稳定介质中恒定背景的一般扰动的长期行为。

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