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A linearized energy-conservative finite element method for the nonlinear Schrodinger equation with wave operator

机译:带波动算子的非线性薛定inger方程的线性守恒有限元方法

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摘要

In this paper, we propose a linearized finite element method (FEM) for solving the cubic nonlinear Schrodinger equation with wave operator. In this method, a modified leapfrog scheme is applied for time discretization and a Galerkin finite element method is applied for spatial discretization. We prove that the proposed method keeps the energy conservation in the given discrete norm. Comparing with non-conservative schemes, our algorithm keeps higher stability. Meanwhile, an optimal error estimate for the proposed scheme is given by an error splitting technique. That is, we split the error into two parts, one from temporal discretization and the other from spatial discretization. First, by introducing a time-discrete system, we prove the uniform boundedness for the solution of this time-discrete system in some strong norms and obtain error estimates in temporal direction. With the help of the preliminary temporal estimates, we then prove the pointwise uniform boundedness of the finite element solution, and obtain the optimal L-2 - norm error estimates in the sense that the time step size is not related to spatial mesh size. Finally, numerical examples are provided to validate the convergence-order, unconditional stability and energy conservation. (C) 2019 Published by Elsevier B.V. on behalf of IMACS.
机译:在本文中,我们提出了一种线性有限元方法(FEM),用于用波动算子求解三次非线性薛定inger方程。在这种方法中,将改进的跳越方案应用于时间离散化,并将Galerkin有限元方法应用于空间离散化。我们证明了该方法在给定的离散范数下保持了能量守恒。与非保守方案相比,我们的算法保持较高的稳定性。同时,通过错误分割技术给出了所提出方案的最佳错误估计。也就是说,我们将误差分为两部分,一部分来自时间离散化,另一部分来自空间离散化。首先,通过引入时离散系统,我们证明了该时离散系统在一些强范数上的一致有界性,并获得了时间方向上的误差估计。借助于初步的时间估计,我们然后证明了有限元解的逐点均匀有界性,并从时间步长大小与空间网格大小无关的意义上获得了最佳的L-2-范数误差估计。最后,通过数值算例验证了收敛阶,无条件稳定性和节能性。 (C)2019由Elsevier B.V.代表IMACS发布。

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