{"title":"用于太阳系外行星探测的旋转剪切干涉仪星光抑制","authors":"M. Scholl","doi":"10.1364/srs.1995.rtue2","DOIUrl":null,"url":null,"abstract":"Star light, scattered from even most smoothly polished optical surfaces, prevents detection of a faint planet light because of the enormous brightness ratio between them. Figure 1 shows two point sources: a dark (Earth-like) planet rotates slowly around a bright star. At the time of observation the planet is assumed to be on x-axis. The wavefronts originating from the star and the planet, respectively, are incident on the aperture at a distant observation plane as plane waves with the propagation vector parallel to the optical axis and tilted with the direction cosine vector (1, 0, n).","PeriodicalId":184407,"journal":{"name":"Signal Recovery and Synthesis","volume":"42 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"4","resultStr":"{\"title\":\"Star-Light Suppression with a rotating Rotational-Shearing Interferometer for Extra-Solar Planet Detection\",\"authors\":\"M. Scholl\",\"doi\":\"10.1364/srs.1995.rtue2\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Star light, scattered from even most smoothly polished optical surfaces, prevents detection of a faint planet light because of the enormous brightness ratio between them. Figure 1 shows two point sources: a dark (Earth-like) planet rotates slowly around a bright star. At the time of observation the planet is assumed to be on x-axis. The wavefronts originating from the star and the planet, respectively, are incident on the aperture at a distant observation plane as plane waves with the propagation vector parallel to the optical axis and tilted with the direction cosine vector (1, 0, n).\",\"PeriodicalId\":184407,\"journal\":{\"name\":\"Signal Recovery and Synthesis\",\"volume\":\"42 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"4\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Signal Recovery and Synthesis\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/srs.1995.rtue2\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Signal Recovery and Synthesis","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/srs.1995.rtue2","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Star-Light Suppression with a rotating Rotational-Shearing Interferometer for Extra-Solar Planet Detection
Star light, scattered from even most smoothly polished optical surfaces, prevents detection of a faint planet light because of the enormous brightness ratio between them. Figure 1 shows two point sources: a dark (Earth-like) planet rotates slowly around a bright star. At the time of observation the planet is assumed to be on x-axis. The wavefronts originating from the star and the planet, respectively, are incident on the aperture at a distant observation plane as plane waves with the propagation vector parallel to the optical axis and tilted with the direction cosine vector (1, 0, n).