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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sg-ntu-dr.10356-796812020-03-07T13:56:08Z Pentadiagonal alternating-direction-implicit finite-difference time-domain method for two-dimensional Schrödinger equation Tay, Wei Choon Tan, Eng Leong School of Electrical and Electronic Engineering DRNTU::Engineering::Electrical and electronic engineering 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. Accepted version 2014-08-19T08:40:15Z 2019-12-06T13:30:55Z 2014-08-19T08:40:15Z 2019-12-06T13:30:55Z 2014 2014 Journal Article Tay, W. C., & Tan, E. L. (2014). Pentadiagonal alternating-direction-implicit finite-difference time-domain method for two-dimensional Schrödinger equation. Computer Physics Communications, 185(7), 1886–1892. https://hdl.handle.net/10356/79681 http://hdl.handle.net/10220/20345 10.1016/j.cpc.2014.03.014 en Computer physics communications © 2014 Elsevier. This is the author created version of a work that has been peer reviewed and accepted for publication by Computer Physics Communications, Elsevier. It incorporates referee’s comments but changes resulting from the publishing process, such as copyediting, structural formatting, may not be reflected in this document. The published version is available at: [http://dx.doi.org/10.1016/j.cpc.2014.03.014]. 12 p. application/pdf |
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DRNTU::Engineering::Electrical and electronic engineering Tay, Wei Choon Tan, Eng Leong Pentadiagonal alternating-direction-implicit finite-difference time-domain method for two-dimensional Schrödinger equation |
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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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School of Electrical and Electronic Engineering |
author_facet |
School of Electrical and Electronic Engineering Tay, Wei Choon Tan, Eng Leong |
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Article |
author |
Tay, Wei Choon Tan, Eng Leong |
author_sort |
Tay, Wei Choon |
title |
Pentadiagonal alternating-direction-implicit finite-difference time-domain method for two-dimensional Schrödinger equation |
title_short |
Pentadiagonal alternating-direction-implicit finite-difference time-domain method for two-dimensional Schrödinger equation |
title_full |
Pentadiagonal alternating-direction-implicit finite-difference time-domain method for two-dimensional Schrödinger equation |
title_fullStr |
Pentadiagonal alternating-direction-implicit finite-difference time-domain method for two-dimensional Schrödinger equation |
title_full_unstemmed |
Pentadiagonal alternating-direction-implicit finite-difference time-domain method for two-dimensional Schrödinger equation |
title_sort |
pentadiagonal alternating-direction-implicit finite-difference time-domain method for two-dimensional schrödinger equation |
publishDate |
2014 |
url |
https://hdl.handle.net/10356/79681 http://hdl.handle.net/10220/20345 |
_version_ |
1681034033672224768 |