Pentadiagonal alternating-direction-implicit finite-difference time-domain method for two-dimensional Schrödinger equation
In this paper, we have proposed a pentadiagonal alternating-direction-implicit (Penta-ADI) finite-difference time-domain (FDTD) method for the two-dimensional Schr¨odinger equation. Through the separation of complex wave function into real and imaginary parts, a pentadiagonal system of equations f...
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Main Authors: | , |
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Other Authors: | |
Format: | Article |
Language: | English |
Published: |
2014
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Subjects: | |
Online Access: | https://hdl.handle.net/10356/79681 http://hdl.handle.net/10220/20345 |
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Institution: | Nanyang Technological University |
Language: | English |
Summary: | In this paper, we have proposed a pentadiagonal alternating-direction-implicit (Penta-ADI) finite-difference
time-domain (FDTD) method for the two-dimensional Schr¨odinger 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 right-hand-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. |
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