完整後設資料紀錄
DC 欄位 | 值 | 語言 |
---|---|---|
dc.contributor.author | Hwang, Jiunn-Nan | en_US |
dc.contributor.author | Chen, Fu-Chiarng | en_US |
dc.date.accessioned | 2014-12-08T15:36:47Z | - |
dc.date.available | 2014-12-08T15:36:47Z | - |
dc.date.issued | 2014-11-01 | en_US |
dc.identifier.issn | 0895-2477 | en_US |
dc.identifier.uri | http://dx.doi.org/10.1002/mop.28658 | en_US |
dc.identifier.uri | http://hdl.handle.net/11536/25155 | - |
dc.description.abstract | The alternating direction implicit-finite-difference time-domain (ADI-FDTD) method can be seen as a second-order perturbation of the Crank-Nicolson FDTD (CN-FDTD) scheme. When the PML is introduced for the ADI-FDTD method, the perturbation term will affect the stability of the ADI-FDTD method. In this work, the stability analysis of the PML schemes for the ADI-FDTD and CN-FDTD are demonstrated. It is found that the PML equations for ADI-FDTD method will be unstable due to the perturbation term. (C) 2014 Wiley Periodicals, Inc. | en_US |
dc.language.iso | en_US | en_US |
dc.subject | Crank-Nicolson FDTD | en_US |
dc.subject | alternating direction implicit-finite-difference time-domain | en_US |
dc.subject | PML | en_US |
dc.subject | stability | en_US |
dc.subject | perturbation term | en_US |
dc.title | STABILITY ANALYSIS OF THE PML SCHEME FOR CN-FDTD AND ADI-FDTD | en_US |
dc.type | Article | en_US |
dc.identifier.doi | 10.1002/mop.28658 | en_US |
dc.identifier.journal | MICROWAVE AND OPTICAL TECHNOLOGY LETTERS | en_US |
dc.citation.volume | 56 | en_US |
dc.citation.issue | 11 | en_US |
dc.citation.spage | 2637 | en_US |
dc.citation.epage | 2642 | en_US |
dc.contributor.department | 交大名義發表 | zh_TW |
dc.contributor.department | 電機工程學系 | zh_TW |
dc.contributor.department | National Chiao Tung University | en_US |
dc.contributor.department | Department of Electrical and Computer Engineering | en_US |
dc.identifier.wosnumber | WOS:000341505400044 | - |
dc.citation.woscount | 0 | - |
顯示於類別: | 期刊論文 |