{"title":"棱镜耦合结构中激发表面等离子体模的线建模方法","authors":"S. Chattopadhyay, P. K. Saha","doi":"10.23919/URSIAP-RASC.2019.8738460","DOIUrl":null,"url":null,"abstract":"Dispersion of propagation constants of Surface Plasmon Polariton (SPP) modes at a metal-dielectric interface with the thickness of buffer layer in both the Otto and the Kretschmann-Raether configurations has been modeled using Method of Lines (MOL). The results reaffirm that in either configurations, the excited mode may not have the desired surface plasmon characteristics if the buffer-layer thickness is too small.","PeriodicalId":344386,"journal":{"name":"2019 URSI Asia-Pacific Radio Science Conference (AP-RASC)","volume":"102 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-03-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Method of Lines Modeling of Surface Plasmon Modes Excited in Prism-Coupled Configurations\",\"authors\":\"S. Chattopadhyay, P. K. Saha\",\"doi\":\"10.23919/URSIAP-RASC.2019.8738460\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Dispersion of propagation constants of Surface Plasmon Polariton (SPP) modes at a metal-dielectric interface with the thickness of buffer layer in both the Otto and the Kretschmann-Raether configurations has been modeled using Method of Lines (MOL). The results reaffirm that in either configurations, the excited mode may not have the desired surface plasmon characteristics if the buffer-layer thickness is too small.\",\"PeriodicalId\":344386,\"journal\":{\"name\":\"2019 URSI Asia-Pacific Radio Science Conference (AP-RASC)\",\"volume\":\"102 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-03-09\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2019 URSI Asia-Pacific Radio Science Conference (AP-RASC)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.23919/URSIAP-RASC.2019.8738460\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2019 URSI Asia-Pacific Radio Science Conference (AP-RASC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.23919/URSIAP-RASC.2019.8738460","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Method of Lines Modeling of Surface Plasmon Modes Excited in Prism-Coupled Configurations
Dispersion of propagation constants of Surface Plasmon Polariton (SPP) modes at a metal-dielectric interface with the thickness of buffer layer in both the Otto and the Kretschmann-Raether configurations has been modeled using Method of Lines (MOL). The results reaffirm that in either configurations, the excited mode may not have the desired surface plasmon characteristics if the buffer-layer thickness is too small.