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Uniform point-wise error estimates of semi-implicit compact finite difference methods for the nonlinear Schrodinger equation perturbed by wave operator

机译:波动算子扰动的非线性Schrodinger方程的半隐式紧致有限差分方法的均匀点误差估计

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摘要

This study is devoted to analysis of semi-implicit compact finite difference (SICFD) methods for the nonlinear Schrodinger equation (NLS) perturbed by the wave operator (NLSW) with a perturbation strength described by a dimensionless parameter epsilon is an element of (0, 1]. Uniform l(infinity)-norm error bounds of the proposed SICFD schemes are built to give immediate insight on point-wise error occurring as time increases, and the explicit dependence of the mesh size and time step on the parameter a is also figured out. In the small is an element of regime, highly oscillations arise in time with O(epsilon(2))-wavelength. This highly oscillatory nature in time as well as the difficulty raised by the compact FD discretization make establishing the l(infinity)-norm error bounds uniformly in a of the SICFD methods for NLSW to be a very interesting and challenging issue. The uniform l(infinity)-norm error bounds in a are proved to be of O(h(4) + tau) and O(h(4) + tau(2/3)) with time step tau and mesh size h for well-prepared and ill-prepared initial data. Finally, numerical results are reported to verify the error estimates and show the sharpness of the convergence rates in the respectively parameter regimes. (C) 2014 Elsevier Inc. All rights reserved.
机译:这项研究致力于分析由波动算子(NLSW)扰动的非线性Schrodinger方程(NLS)的半隐式有限差分(SICFD)方法,其扰动强度由无量纲参数epsilon表示为(0, 1]。提出的SICFD方案的一致l(无穷)-范数误差范围可立即了解随着时间增加而发生的逐点误差,并且网格大小和时间步长对参数a的显式依赖也在很小的范围内,随着O(epsilon(2))波长的变化,时间上会出现高度振荡,这种时间上的高度振荡以及紧凑的FD离散化带来的困难使得建立l( NLSW的SICFD方法中的a)的均匀无穷范数误差界限是一个非常有趣且具有挑战性的问题,a中的均匀l(无穷大)范数误差界限证明为O(h(4)+ tau)和O(h(4)+ tau(2/3))随时间变化准备好和准备不好的初始数据的tau和网格大小h。最后,报告了数值结果以验证误差估计并显示在各个参数方案中收敛速度的清晰度。 (C)2014 Elsevier Inc.保留所有权利。

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