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On the efficiency of different numerical methods for the calculation of intrapulse Raman scattering of optical solitons

机译:关于不同数值方法的效率计算光学孤子的intapulse拉曼散射

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摘要

In this paper we compare the performance of different numerical methods for the calculation of the asymptotic evolution of soliton self-frequency shift in the presence of intrapulse Raman scattering (IRS) in optical fibers. First we have calculated the order of global accuracy for the fundamental soliton and the second-order bound state of the unperturbed nonlinear Schrodinger equation for the following numerical methods: the simple split step (SS) method, the full SS method, the reduced SS method, the reduced SS method with fourth order Runge-Kutta (RK4), the Blow-Wood method, the fourth order Runge-Kutta in the interaction picture (RK4IP) method and the Agrawal SS method with one and two iterations. We have shown that the asymptotic evolution of soliton self-frequency shift in the presence of IRS in optical fiber can be best described by the Agrawal SS method (compared to the Blow-Wood method and the RK4IP method). The obtained numerical results for the soliton position and frequency are in agreement with the predictions for these parameters according to the perturbation theory. We have shown that in the presence of IRS the fundamental soliton quickly develops an oscillating tail on its left. The generated tail hardly influences the soliton propagation at large distances. At large distances the form of the soliton gradually becomes asymmetric. The increase of the frequency resolution leads to a notable increase of the maximum propagation distance of the numerical soliton under the influence of IRS.
机译:在本文中,我们比较了不同数值方法的性能来计算孤子自频在光纤中的内侧射击散射(IRS)存在下孤子自频偏移的渐近演变。首先,我们已经计算了基本孤子的全球精度的顺序,并且对于未受干扰的非线性Schrodinger方程的二阶绑定状态,用于以下数值方法:简单的分流步骤(SS)方法,全SS方法,减少的SS方法,具有四阶runge-Kutta(RK4)的SS方法,吹木工方法,交互图像中的第四阶runge-Kutta(RK4IP)方法和具有一个和两个迭代的Agrawal SS方法。我们已经表明,在光纤中的IRS存在下孤子自频移位的渐近进化可以最好地由Agrawal SS方法描述(与吹木材方法和RK4IP方法相比)。根据扰动理论,孤子位置和频率的所得数值结果与这些参数的预测一致。我们已经表明,在IRS的存在中,基本孤独的孤子迅速在左侧开发振荡尾部。产生的尾部几乎不影响大距离的孤子繁殖。在大距离孤子的形式逐渐变得不对称。频率分辨率的增加导致在IRS的影响下的数值孤子的最大传播距离的显着增加。

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