论文标题
方程式的第二阶准确标量辅助变量(SAV)数值方法
A second order accurate scalar auxiliary variable (SAV) numerical method for the square phase field crystal equation
论文作者
论文摘要
在本文中,我们提出和分析了平方相场晶体(SPFC)方程的二阶准确(时间)数值方案,这是空间中原子尺度上的梯度流量建模晶体动力学,但在时间上进行扩散尺度。它与标准相场晶体模型的主要区别是在自由能电位中引入了4-Laplacian项,这又导致了更高的非线性程度。为了使数值方案在保留非线性能量稳定性时进行线性,我们使用标量辅助变量(SAV)方法,其中二阶向后分化公式(BDF)在时间模板中应用。同时,由于4-Laplacian项的参与,SAV方法的直接应用面临某些困难,并结合了非线性能量功能的下限的推导。在拟议的数值方法中,制定了针对物理能函数的适当分解,以使非线性能量部分具有完善的全局下限,其余项会导致具有正征值的恒定式扩散项。反过来,数值方案可以通过恒定的类似泊松型型求解器(通过FFT)非常有效地实现,并且通过引入辅助变量来确定能量稳定性,并为提出的SAV方法提供了最佳速率收敛分析。还提供了一些数值实验,这些实验证实了所提出的方案的效率和准确性。
In this paper we propose and analyze a second order accurate (in time) numerical scheme for the square phase field crystal (SPFC) equation, a gradient flow modeling crystal dynamics at the atomic scale in space but on diffusive scales in time. Its primary difference with the standard phase field crystal model is an introduction of the 4-Laplacian term in the free energy potential, which in turn leads to a much higher degree of nonlinearity. To make the numerical scheme linear while preserving the nonlinear energy stability, we make use of the scalar auxiliary variable (SAV) approach, in which a second order backward differentiation formula (BDF) is applied in the temporal stencil. Meanwhile, a direct application of the SAV method faces certain difficulties, due to the involvement of the 4-Laplacian term, combined with a derivation of the lower bound of the nonlinear energy functional. In the proposed numerical method, an appropriate decomposition for the physical energy functional is formulated, so that the nonlinear energy part has a well-established global lower bound, and the rest terms lead to constant-coefficient diffusion terms with positive eigenvalues. In turn, the numerical scheme could be very efficiently implemented by constant-coefficient Poisson-like type solvers (via FFT), and energy stability is established by introducing an auxiliary variable, and an optimal rate convergence analysis is provided for the proposed SAV method. A few numerical experiments are also presented, which confirm the efficiency and accuracy of the proposed scheme.