{"title":"Orthogonal decomposition of external oscillation","authors":"H. Xu, W. Wang","doi":"10.1109/APS.1988.94167","DOIUrl":null,"url":null,"abstract":"External oscillation is decomposed orthogonally using the theory of differential geometry. It is shown that the SEM (singularity expansion method) poles of a smooth scatterer in three-dimension have three indexes (l, m, n). The l indicates the order of the creeping wave on the surface, and m and n describe the modes of the standing waves in two orthogonal directions. It is noted that the SEM poles of a sphere have two indexes (l, n); for a smooth scatterer, the index number of SEM poles is the same as the dimension number of the oscillation trajectory, but for a scatterer having nonsmooth points on the trajectory the index number of SEM poles will be larger, because the diffraction fields caused by these points have a number of orders.<<ETX>>","PeriodicalId":211271,"journal":{"name":"1988 IEEE AP-S. International Symposium, Antennas and Propagation","volume":"220 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1988-06-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"1988 IEEE AP-S. International Symposium, Antennas and Propagation","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/APS.1988.94167","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
Abstract
External oscillation is decomposed orthogonally using the theory of differential geometry. It is shown that the SEM (singularity expansion method) poles of a smooth scatterer in three-dimension have three indexes (l, m, n). The l indicates the order of the creeping wave on the surface, and m and n describe the modes of the standing waves in two orthogonal directions. It is noted that the SEM poles of a sphere have two indexes (l, n); for a smooth scatterer, the index number of SEM poles is the same as the dimension number of the oscillation trajectory, but for a scatterer having nonsmooth points on the trajectory the index number of SEM poles will be larger, because the diffraction fields caused by these points have a number of orders.<>