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arXiv 1401.0984math.NAcs.NA
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一种适用于Klein-Gordon方程非相对论极限区域的统一准确多尺度时间积分伪谱方法

A uniformly accurate multiscale time integrator pseudospectral method for the Klein-Gordon equation in the nonrelativistic limit regime

National University of Singapore(新加坡国立大学);Purdue University(普渡大学)

Weizhu Bao, Yongyong Cai, Xiaofei Zhao

AI总结:

本文提出并分析了一种多尺度时间积分傅里叶伪谱方法,用于求解具有无量纲参数0<ε≤1的Klein-Gordon方程,在非相对论极限区域中,该方法通过多尺度分解和指数波积分器有效处理高振荡问题,证明了其在空间和时间上的统一最优收敛性。

摘要:

我们提出并分析了一种多尺度时间积分傅里叶伪谱(MTI-FP)方法,用于求解具有无量纲参数0<ε≤1的Klein-Gordon(KG)方程,该参数与光速成反比。在非相对论极限区域,即0<ε<<1时,KG方程的解在时间和空间上分别传播振幅为O(1)、波长为O(ε²)的波,这导致了显著的数值负担,因为时间上的高振荡。MTI-FP方法通过在每个时间步将解进行多尺度分解,并应用指数波积分器到非线性薛定谔方程(带有波算子)和KG型方程,以处理ε²频率和O(1)振幅的波,以及小初始数据的剩余波。我们严格建立了两种独立的误差界,分别在H²范数下为O(h^{m0}+τ²+ε²)和O(h^{m0}+τ²/ε²),其中h是网格尺寸,τ是时间步长,m0≥2是取决于解正则性的整数。这立即表明,如果解是光滑的,MTI-FP在空间上以指数收敛率统一且最优地收敛,并在时间上以线性收敛率O(τ)统一收敛于所有ε∈(0,1],在ε=O(1)或0<ε≤τ的区域中则以二次收敛率O(τ²)最优。数值结果证实了误差界,并展示了MTI-FP方法在KG方程,特别是非相对论极限区域中的效率和准确性。

英文摘要:

We propose and analyze a multiscale time integrator Fourier pseudospectral (MTI-FP) method for solving the Klein-Gordon (KG) equation with a dimensionless parameter $0<\varepsilon\leq1$ which is inversely proportional to the speed of light. In the nonrelativistic limit regime, i.e. $0<\varepsilon\ll1$, the solution to the KG equation propagates waves with amplitude at $O(1)$ and wavelength at $O(\varepsilon^2)$ in time and $O(1)$ in space, which causes significantly numerical burdens due to the high oscillation in time. The MTI-FP method is designed by adapting a multiscale decomposition by frequency (MDF) to the solution at each time step and applying an exponential wave integrator to the nonlinear Schrödinger equation with wave operator under well-prepared initial data for $\varepsilon^2$-frequency and $O(1)$-amplitude waves and a KG-type equation with small initial data for the reminder waves in the MDF. We rigorously establish two independent error bounds in $H^2$-norm to the MTI-FP method at $O(h^{m_0}+τ^2+\varepsilon^2)$ and $O(h^{m_0}+τ^2/\varepsilon^2)$ with $h$ mesh size, $τ$ time step and $m_0\ge2$ an integer depending on the regularity of the solution, which immediately imply that the MTI-FP converges uniformly and optimally in space with exponential convergence rate if the solution is smooth, and uniformly in time with linear convergence rate at $O(τ)$ for all $\varepsilon\in(0,1]$ and optimally with quadratic convergence rate at $O(τ^2)$ in the regimes when either $\varepsilon=O(1)$ or $0<\varepsilon\le τ$. Numerical results are reported to confirm the error bounds and demonstrate the efficiency and accuracy of the MTI-FP method for the KG equation, especially in the nonrelativistic limit regime.

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