{"title":"大粗糙度表面的光谱椭偏测量","authors":"L. Melnichenko, B. B. Tytarchuk, I. A. Shaykevich","doi":"10.1117/12.486670","DOIUrl":null,"url":null,"abstract":"Spectroellipsometrical measurements are usually made on smooth surfaces or surfaces with small roughness. Practical needs often demand measuring optical parameters of real details and products. The surface of these dtails and products is not mirror-like, but veyr rough, that is Ra greater than/equal to λ. This work shows possibility of ellipsometrical measurements on very rough surfaces. We proposed the method of ellipsometrical measurement of these surfaces and made investigations for metal rough plates and semiconductor surfaces of the anodized aluminum. The most common method of measurement of spectroellipsometrical parameters is the Beatty method and its different modifications. Therefore it is for this method that we work out our own principles.","PeriodicalId":205850,"journal":{"name":"International School on Spectroscopy of Molecules and Crystals","volume":"333 ","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2002-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Spectroellipsometrical measurement of large roughness surface\",\"authors\":\"L. Melnichenko, B. B. Tytarchuk, I. A. Shaykevich\",\"doi\":\"10.1117/12.486670\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Spectroellipsometrical measurements are usually made on smooth surfaces or surfaces with small roughness. Practical needs often demand measuring optical parameters of real details and products. The surface of these dtails and products is not mirror-like, but veyr rough, that is Ra greater than/equal to λ. This work shows possibility of ellipsometrical measurements on very rough surfaces. We proposed the method of ellipsometrical measurement of these surfaces and made investigations for metal rough plates and semiconductor surfaces of the anodized aluminum. The most common method of measurement of spectroellipsometrical parameters is the Beatty method and its different modifications. Therefore it is for this method that we work out our own principles.\",\"PeriodicalId\":205850,\"journal\":{\"name\":\"International School on Spectroscopy of Molecules and Crystals\",\"volume\":\"333 \",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2002-12-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International School on Spectroscopy of Molecules and Crystals\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1117/12.486670\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International School on Spectroscopy of Molecules and Crystals","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1117/12.486670","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Spectroellipsometrical measurement of large roughness surface
Spectroellipsometrical measurements are usually made on smooth surfaces or surfaces with small roughness. Practical needs often demand measuring optical parameters of real details and products. The surface of these dtails and products is not mirror-like, but veyr rough, that is Ra greater than/equal to λ. This work shows possibility of ellipsometrical measurements on very rough surfaces. We proposed the method of ellipsometrical measurement of these surfaces and made investigations for metal rough plates and semiconductor surfaces of the anodized aluminum. The most common method of measurement of spectroellipsometrical parameters is the Beatty method and its different modifications. Therefore it is for this method that we work out our own principles.