{"title":"空气-二氧化硅微结构波导的倏逝场分析[用于生物传感应用]","authors":"B. Gibson, J. Love, L. Cahill, P. Dower, D. Elton","doi":"10.1109/LEOS.2001.969011","DOIUrl":null,"url":null,"abstract":"A comprehensive analytical and numerical study of the fraction of evanescent modal power and the fraction of modal power in the holes has been presented for air-silica microstructures. It was shown for the 4-layer structures, that when the waveguide half width was kept constant and a was varied between 0 and s/2, the fraction of modal power in regions 2 and 4 was greater in the case of the periodic waveguide than the waveguide with the core region. This was a result of the core region have a confining effect on the mode. It was also determined that by adding another air-silica layer to the 4-layer structure, the fraction of evanescent power and power in the holes was increased for all values of a So, the ideal waveguide characteristics of a periodic 6-layer air-silica microstructure that maximises the power in the holes and evanescent power for biosensing applications is to have a as large as mechanically possible (i.e. large holes).","PeriodicalId":18008,"journal":{"name":"LEOS 2001. 14th Annual Meeting of the IEEE Lasers and Electro-Optics Society (Cat. No.01CH37242)","volume":"23 1","pages":"709-710 vol.2"},"PeriodicalIF":0.0000,"publicationDate":"2001-11-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"7","resultStr":"{\"title\":\"Evanescent field analysis of air-silica microstructure waveguides [for biosensing applications]\",\"authors\":\"B. Gibson, J. Love, L. Cahill, P. Dower, D. Elton\",\"doi\":\"10.1109/LEOS.2001.969011\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A comprehensive analytical and numerical study of the fraction of evanescent modal power and the fraction of modal power in the holes has been presented for air-silica microstructures. It was shown for the 4-layer structures, that when the waveguide half width was kept constant and a was varied between 0 and s/2, the fraction of modal power in regions 2 and 4 was greater in the case of the periodic waveguide than the waveguide with the core region. This was a result of the core region have a confining effect on the mode. It was also determined that by adding another air-silica layer to the 4-layer structure, the fraction of evanescent power and power in the holes was increased for all values of a So, the ideal waveguide characteristics of a periodic 6-layer air-silica microstructure that maximises the power in the holes and evanescent power for biosensing applications is to have a as large as mechanically possible (i.e. large holes).\",\"PeriodicalId\":18008,\"journal\":{\"name\":\"LEOS 2001. 14th Annual Meeting of the IEEE Lasers and Electro-Optics Society (Cat. No.01CH37242)\",\"volume\":\"23 1\",\"pages\":\"709-710 vol.2\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2001-11-12\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"7\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"LEOS 2001. 14th Annual Meeting of the IEEE Lasers and Electro-Optics Society (Cat. No.01CH37242)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/LEOS.2001.969011\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"LEOS 2001. 14th Annual Meeting of the IEEE Lasers and Electro-Optics Society (Cat. No.01CH37242)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/LEOS.2001.969011","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Evanescent field analysis of air-silica microstructure waveguides [for biosensing applications]
A comprehensive analytical and numerical study of the fraction of evanescent modal power and the fraction of modal power in the holes has been presented for air-silica microstructures. It was shown for the 4-layer structures, that when the waveguide half width was kept constant and a was varied between 0 and s/2, the fraction of modal power in regions 2 and 4 was greater in the case of the periodic waveguide than the waveguide with the core region. This was a result of the core region have a confining effect on the mode. It was also determined that by adding another air-silica layer to the 4-layer structure, the fraction of evanescent power and power in the holes was increased for all values of a So, the ideal waveguide characteristics of a periodic 6-layer air-silica microstructure that maximises the power in the holes and evanescent power for biosensing applications is to have a as large as mechanically possible (i.e. large holes).