{"title":"广义Harvey-Shack表面散射理论","authors":"A. Krywonos","doi":"10.1117/3.2530114.CH5","DOIUrl":null,"url":null,"abstract":"Surface scatter of electromagnetic radiation is not caused directly by surface roughness, but rather by the effect of the phase variation induced on the transmitted or reflected wavefront as it propagates; i.e., surface scatter is a diffraction phenomenon caused directly by the propagation process. The scatter behavior is thus strongly affected by: (1) the statistical nature of the surface, (2) the propagating wavelength, (3) the angle of incidence, and (4) the refractive index of the media both before and after the interface of the surface encountered.","PeriodicalId":347238,"journal":{"name":"Understanding Surface Scatter: A Linear Systems Formulation","volume":"71 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-07-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The Generalized Harvey–Shack Surface Scatter Theory\",\"authors\":\"A. Krywonos\",\"doi\":\"10.1117/3.2530114.CH5\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Surface scatter of electromagnetic radiation is not caused directly by surface roughness, but rather by the effect of the phase variation induced on the transmitted or reflected wavefront as it propagates; i.e., surface scatter is a diffraction phenomenon caused directly by the propagation process. The scatter behavior is thus strongly affected by: (1) the statistical nature of the surface, (2) the propagating wavelength, (3) the angle of incidence, and (4) the refractive index of the media both before and after the interface of the surface encountered.\",\"PeriodicalId\":347238,\"journal\":{\"name\":\"Understanding Surface Scatter: A Linear Systems Formulation\",\"volume\":\"71 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-07-31\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Understanding Surface Scatter: A Linear Systems Formulation\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1117/3.2530114.CH5\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Understanding Surface Scatter: A Linear Systems Formulation","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1117/3.2530114.CH5","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The Generalized Harvey–Shack Surface Scatter Theory
Surface scatter of electromagnetic radiation is not caused directly by surface roughness, but rather by the effect of the phase variation induced on the transmitted or reflected wavefront as it propagates; i.e., surface scatter is a diffraction phenomenon caused directly by the propagation process. The scatter behavior is thus strongly affected by: (1) the statistical nature of the surface, (2) the propagating wavelength, (3) the angle of incidence, and (4) the refractive index of the media both before and after the interface of the surface encountered.