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: Tay, Wei Choon, Tan, Eng Leong
Other Authors: School of Electrical and Electronic Engineering
Format: Article
Language:English
Published: 2014
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Online Access:https://hdl.handle.net/10356/79681
http://hdl.handle.net/10220/20345
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Institution: Nanyang Technological University
Language: English
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spelling 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
institution Nanyang Technological University
building NTU Library
country Singapore
collection DR-NTU
language English
topic DRNTU::Engineering::Electrical and electronic engineering
spellingShingle 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
description 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.
author2 School of Electrical and Electronic Engineering
author_facet School of Electrical and Electronic Engineering
Tay, Wei Choon
Tan, Eng Leong
format 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