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The GLM representation of the global relation for the two-component nonlinear Schrodinger equation on the interval

机译:间隔双组分非线性Schrodinger方程的全局关系的GLM表示

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In a previous work, we show that the solution of the initial-boundary value problem for the two-component nonlinear Schrodinger equation on the finite interval can be expressed in terms of the solution of a 3 x 3 Riemann-Hilbert problem. The relevant jump matrices are explicitly given in terms of the three matrix-value spectral functions s(k), S(k), and SL(k), which in turn are defined in terms of the initial values, boundary values at x = 0, and boundary values at x = L, respectively. However, for a wellposed problem, only part of the boundary values can be prescribed, the remaining boundary data cannot be independently specified but are determined by the so-called global relation. Here, we use a Gelfand-Levitan-Marchenko representation to derive an expression for the generalized Dirichlet-to-Neumann map to characterize the unknown boundary values in physical domain, which is different from the approach, in fact it analyzed the global relation in spectral domain, used in the previous work. And, we can show that these two representations are equivalent. Published by AIP Publishing.
机译:在以前的工作中,我们表明,在有限间隔内的双组分非线性Schrodinger方程的初始边界值问题的解决方案可以以3×3 riemann-hilbert问题的解决方案来表达。根据三个矩阵值频谱函数S(k),s(k)和sl(k)明确地给出相关的跳跃矩阵,SL(k)又在初始值方面定义,X =的边界值0,分别为x = l的边界值。然而,对于井斑问题,只有部分边界值可以规定,剩余的边界数据不能独立地指定,而是由所谓的全局关系确定。在这里,我们使用Gelfand-Levitan-Marchenko表示来导出概括的Dirichlet-neumann地图的表达式,以表征物理域中的未知边界值,这与方法不同,实际上它分析了频谱中的全局关系域,用于上一个工作。而且,我们可以表明这两个表示是等同的。通过AIP发布发布。

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