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Bright-soliton collisions with shape change by intensity redistribution for the coupled Sasa-Satsuma system in the optical fiber communications

机译:光纤通信中耦合的Sasa-Satsuma系统通过强度重新分布而发生形状改变的亮孤子碰撞

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By means of symbolic computation and Darboux transformation, analytically and numerically investigated in this paper is a two-coupled Sasa-Satsuma system, which can describe the pulse propagation in birefringent fibers, so as to increase the bit rate in optical fibers, or achieve wavelength-division multiplexing. Analytical bright N-soliton solution of the system is firstly derived. Based on the bright one- and two-soliton solutions, numerical simulation and figure illustration are carried out on through the multi-parametric management, i.e., different choices among eight parameters in the two-soliton solutions. The interaction mechanisms for the bright two-solitons are revealed in three aspects: Separating evolution behaviors, elastic collision behaviors and inelastic collision behaviors. There exist three different cases for the inelastic collision for the two-soliton, which reflect correspondingly different energy transfer mechanisms (by intensity redistribution) between the two components: Manakov-typed collision; a near-elastic collision and another completely inelastic collision between the two components; and four single-soli-tons in two components undergo shape changes (inelastic and elastic) due to intensity redistribution, where one single-soliton keeps invariant and the other three single-solitons change during the collision. The collision mechanisms may be viewed as the two-solitons interact in a waveguide supporting propagation of two nonlinear waves simultaneously. In general, partial suppression (enhancement) of intensity between the components is dependent on the values of the soliton parameters.
机译:通过符号计算和Darboux变换,本文通过分析和数值研究了一种双耦合的Sasa-Satsuma系统,该系统可以描述双折射光纤中的脉冲传播,从而增加光纤中的比特率或达到波长分区复用。首先推导了该系统的解析亮N孤子解。在明亮的一孤子和二孤子解决方案的基础上,通过多参数管理,即在二孤子解决方案的八个参数中进行不同选择,进行了数值模拟和图形说明。从三个方面揭示了明亮的两个孤子的相互作用机理:分离演化行为,弹性碰撞行为和非弹性碰撞行为。两孤子的非弹性碰撞存在三种不同的情况,它们反映了两个分量之间相应的不同的能量传递机制(通过强度重新分布):马纳科夫型碰撞;这两个组件之间存在接近弹性的碰撞,而另一个完全是非弹性的碰撞;由于强度重新分布,两个分量中的四个单孤子会发生形状变化(弹性和弹性),其中一个单孤子保持不变,而其他三个单孤子在碰撞过程中发生变化。碰撞机理可以看作是两个孤子在波导中相互作用,同时支持两个非线性波的传播。通常,分量之间的强度的部分抑制(增强)取决于孤子参数的值。

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