{"title":"Alternating-direction explicit FDTD method for three-dimensional full-wave simulation","authors":"S. Aono, M. Unno, H. Asai","doi":"10.1109/ECTC.2010.5490946","DOIUrl":null,"url":null,"abstract":"In this paper, we propose a new FDTD (Finite-Difference Time-Domain) method using the alternating-direction explicit (ADE) method for the efficient electromagnetic field simulation. This method is based on the ADE method which has been used as the explicit-type finite-difference algorithm for solving diffusion equations. Our approach is the first application of the ADE method to the 3D-FDTD method. Furthermore, we introduce an absorbing boundary condition suitable for the 3D ADE-FDTD method which has been modified from the PML (perfectly matched layer). Finally, the efficiency of the ADE-FDTD method is evaluated by computer simulations.","PeriodicalId":429629,"journal":{"name":"2010 Proceedings 60th Electronic Components and Technology Conference (ECTC)","volume":"794 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2010-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"9","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2010 Proceedings 60th Electronic Components and Technology Conference (ECTC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ECTC.2010.5490946","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 9
Abstract
In this paper, we propose a new FDTD (Finite-Difference Time-Domain) method using the alternating-direction explicit (ADE) method for the efficient electromagnetic field simulation. This method is based on the ADE method which has been used as the explicit-type finite-difference algorithm for solving diffusion equations. Our approach is the first application of the ADE method to the 3D-FDTD method. Furthermore, we introduce an absorbing boundary condition suitable for the 3D ADE-FDTD method which has been modified from the PML (perfectly matched layer). Finally, the efficiency of the ADE-FDTD method is evaluated by computer simulations.