{"title":"EUV掩模毛坯缺陷光散射模拟","authors":"M. Ito, T. Ogawa, I. Nishiyama, S. Okazaki","doi":"10.1109/IMNC.2001.984093","DOIUrl":null,"url":null,"abstract":"Using light scatter simulations, we have predicted the PSL-equivalent sensitivity needed for mask blank inspection. The simulation procedure has two steps. First, the electromagnetic field scattered off a feature is calculated by solving Maxwell's equations with a time-domain finite-element method. Then, the resultant near field is extrapolated to the far field using the Kirchhoff diffraction formula. We performed two-dimensional simulations at a wavelength of 488 nm (Ar laser). The mask blank is illuminated by an s-polarized plane wave at normal incidence. We also discuss the angular distribution of scattered intensity, as well as the effects of incident angle and wavelength on light scattering.","PeriodicalId":202620,"journal":{"name":"Digest of Papers. Microprocesses and Nanotechnology 2001. 2001 International Microprocesses and Nanotechnology Conference (IEEE Cat. No.01EX468)","volume":"4 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2001-10-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":"{\"title\":\"Simulation of light scatter from defects in EUV mask blanks\",\"authors\":\"M. Ito, T. Ogawa, I. Nishiyama, S. Okazaki\",\"doi\":\"10.1109/IMNC.2001.984093\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Using light scatter simulations, we have predicted the PSL-equivalent sensitivity needed for mask blank inspection. The simulation procedure has two steps. First, the electromagnetic field scattered off a feature is calculated by solving Maxwell's equations with a time-domain finite-element method. Then, the resultant near field is extrapolated to the far field using the Kirchhoff diffraction formula. We performed two-dimensional simulations at a wavelength of 488 nm (Ar laser). The mask blank is illuminated by an s-polarized plane wave at normal incidence. We also discuss the angular distribution of scattered intensity, as well as the effects of incident angle and wavelength on light scattering.\",\"PeriodicalId\":202620,\"journal\":{\"name\":\"Digest of Papers. Microprocesses and Nanotechnology 2001. 2001 International Microprocesses and Nanotechnology Conference (IEEE Cat. No.01EX468)\",\"volume\":\"4 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2001-10-31\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"3\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Digest of Papers. Microprocesses and Nanotechnology 2001. 2001 International Microprocesses and Nanotechnology Conference (IEEE Cat. No.01EX468)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/IMNC.2001.984093\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Digest of Papers. Microprocesses and Nanotechnology 2001. 2001 International Microprocesses and Nanotechnology Conference (IEEE Cat. No.01EX468)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IMNC.2001.984093","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Simulation of light scatter from defects in EUV mask blanks
Using light scatter simulations, we have predicted the PSL-equivalent sensitivity needed for mask blank inspection. The simulation procedure has two steps. First, the electromagnetic field scattered off a feature is calculated by solving Maxwell's equations with a time-domain finite-element method. Then, the resultant near field is extrapolated to the far field using the Kirchhoff diffraction formula. We performed two-dimensional simulations at a wavelength of 488 nm (Ar laser). The mask blank is illuminated by an s-polarized plane wave at normal incidence. We also discuss the angular distribution of scattered intensity, as well as the effects of incident angle and wavelength on light scattering.