Integrable nonlinear ladder system with background-controlled intersite resonant coupling

O. O. Vakhnenko
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引用次数: 26

Abstract

A new spectral problem on one-dimensional lattices is found allowing consistently to support the zero-curvature representation for a wide class of integrable nonlinear ladder systems. The modified recurrence technique for obtaining an infinite set of conservation laws is developed and some basic conserved quantities are explicitly derived. The eigenvalue problems associated with the limiting spectral operator for the special case of rapidly vanishing boundary conditions on Schrödinger-type fields and finite background condition on a concomitant field are solved and the domains of analyticity of Jost functions are presented both analytically and graphically. This particular example shows that the original auxiliary spectral problem is basically of fourth order and must generate a set of four distinct Jost functions that have to be involved in the procedure of inverse scattering transform. Moreover, there exists a critical background value of accompanying field which separates two principally different possibilities in the organization of analyticity domains of Jost functions. This crossover should inevitably lead to qualitative rearrangements in the structure of model solutions. Thus already in the limit of low-amplitude excitations we strictly observe the loss of stability regarding the linear spectrum of Schrödinger subsystem just above the critical background value of practically unexcited concomitant field, whereas in the stability region the structure of linear spectrum is essentially controlled by the magnitude of background level via effective modification of both intersite resonant coupling and self-site coupling.
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具有背景控制局间谐振耦合的可积非线性阶梯系统
对于一类广泛的可积非线性阶梯系统,在一维格上发现了一个新的谱问题,它可以一致地支持零曲率表示。提出了求无限守恒定律集的改进递推法,并明确地导出了一些基本守恒量。求解了Schrödinger-type域上边界条件迅速消失和伴随域上背景条件有限的特殊情况下的极限谱算子的特征值问题,给出了Jost函数的解析域和图解域。这个特殊的例子表明,原始的辅助光谱问题基本上是四阶的,必须产生一个由四个不同的Jost函数组成的集合,这些函数必须参与散射逆变换的过程。此外,在约斯特函数解析域的组织中,存在一个临界伴随场的背景值,它将两种主要不同的可能性分开。这种交叉将不可避免地导致模型解决方案结构的质的重新安排。因此,在低幅激励的极限下,我们已经严格观察到Schrödinger子系统的线性谱在实际未激发伴随场的临界背景值以上的稳定性损失,而在稳定区域,线性谱的结构基本上是通过有效地修改场间谐振耦合和自场耦合来控制背景电平的大小。
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