{"title":"表面等离激元沿金属纳米孔和纳米线的传输特性","authors":"H. X. Yuan, B. Xu, T. Chong","doi":"10.1117/12.685180","DOIUrl":null,"url":null,"abstract":"Surface plasmon propagation properties for nano-sized metal aperture and nano-wire structures are studied based on the waveguide theory. It is verified that there are only TM0 and HE1 mode existing in both structures. For nano-wire structure, however, there is no cut-off radii for both TM0 and HE1 mode. On the contrast, there is a cut-off radius for nano-sized silver aperture structure, and even more, there are several characteristic radius coefficients a/lambda, - 0.32, 0.73. For each section, the EM wave may takes on different features, e.g.. totally-bounded features along the aperture interface for a/lambda > 0.73, or oscillation inside core or strong attenuation along z direction for 0.32 < a/lambda <0.73. HE1 mode of metal aperture doesn't show cutoff radius as well, but the wave-number along z direction monotonically increase with the radius coefficient a/lambda in contrast with existence of a characteristic radius coefficient a/lambda of 0.41 for nano-wire","PeriodicalId":332569,"journal":{"name":"2006 Optical Data Storage Topical Meeting","volume":"4 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2006-06-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Propagation Properties of Surface Plasmon along Metal Nano-Aperture and Nano-Wire\",\"authors\":\"H. X. Yuan, B. Xu, T. Chong\",\"doi\":\"10.1117/12.685180\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Surface plasmon propagation properties for nano-sized metal aperture and nano-wire structures are studied based on the waveguide theory. It is verified that there are only TM0 and HE1 mode existing in both structures. For nano-wire structure, however, there is no cut-off radii for both TM0 and HE1 mode. On the contrast, there is a cut-off radius for nano-sized silver aperture structure, and even more, there are several characteristic radius coefficients a/lambda, - 0.32, 0.73. For each section, the EM wave may takes on different features, e.g.. totally-bounded features along the aperture interface for a/lambda > 0.73, or oscillation inside core or strong attenuation along z direction for 0.32 < a/lambda <0.73. HE1 mode of metal aperture doesn't show cutoff radius as well, but the wave-number along z direction monotonically increase with the radius coefficient a/lambda in contrast with existence of a characteristic radius coefficient a/lambda of 0.41 for nano-wire\",\"PeriodicalId\":332569,\"journal\":{\"name\":\"2006 Optical Data Storage Topical Meeting\",\"volume\":\"4 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2006-06-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2006 Optical Data Storage Topical Meeting\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1117/12.685180\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2006 Optical Data Storage Topical Meeting","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1117/12.685180","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Propagation Properties of Surface Plasmon along Metal Nano-Aperture and Nano-Wire
Surface plasmon propagation properties for nano-sized metal aperture and nano-wire structures are studied based on the waveguide theory. It is verified that there are only TM0 and HE1 mode existing in both structures. For nano-wire structure, however, there is no cut-off radii for both TM0 and HE1 mode. On the contrast, there is a cut-off radius for nano-sized silver aperture structure, and even more, there are several characteristic radius coefficients a/lambda, - 0.32, 0.73. For each section, the EM wave may takes on different features, e.g.. totally-bounded features along the aperture interface for a/lambda > 0.73, or oscillation inside core or strong attenuation along z direction for 0.32 < a/lambda <0.73. HE1 mode of metal aperture doesn't show cutoff radius as well, but the wave-number along z direction monotonically increase with the radius coefficient a/lambda in contrast with existence of a characteristic radius coefficient a/lambda of 0.41 for nano-wire