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Pentadiagonal alternating-direction-implicit finite-difference time-domain method for two-dimensional Schr?dinger equation

机译:五角形交替方向隐式时域有限差分法求解二维薛定r方程

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摘要

In this paper, we have proposed a pentadiagonal alternating-direction-implicit (Penta-ADI) finitedifference time-domain (FDTD) method for the two-dimensional Schr?dinger equation. Through the separation of complex wave function into real and imaginary parts, a pentadiagonal system of equations for the ADI method is obtained, which results in our Penta-ADI method. The Penta-ADI method is further simplified into pentadiagonal fundamental ADI (Penta-FADI) method, which has matrix-operator-free righthand- sides (RHS), leading to the simplest and most concise update equations. As the Penta-FADI method involves five stencils in the left-hand-sides (LHS) of the pentadiagonal update equations, special treatments that are required for the implementation of the Dirichlet's boundary conditions will be discussed. Using the Penta-FADI method, a significantly higher efficiency gain can be achieved over the conventional Tri-ADI method, which involves a tridiagonal system of equations.
机译:在本文中,我们为二维Schr?dinger方程提出了一种五角对角交替方向隐式(Penta-ADI)有限差分时域(FDTD)方法。通过将复波函数分离为实部和虚部,得到了ADI方法的五对角方程组,这就是我们的Penta-ADI方法。 Penta-ADI方法进一步简化为五对角基本ADI(Penta-FADI)方法,该方法具有无矩阵运算符的右手边(RHS),从而得出最简单,最简洁的更新公式。由于Penta-FADI方法在五对角更新方程的左侧(LHS)中包含五个模具,因此将讨论实现Dirichlet边界条件所需的特殊处理。使用Penta-FADI方法,可以比传统的Tri-ADI方法获得更高的效率增益,传统的Tri-ADI方法涉及方程的三对角线系统。

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