{"id":2074,"date":"2021-04-22T11:33:10","date_gmt":"2021-04-22T02:33:10","guid":{"rendered":"http:\/\/uniopt.co.jp\/?page_id=2074"},"modified":"2023-02-13T11:00:53","modified_gmt":"2023-02-13T02:00:53","slug":"sbr-02","status":"publish","type":"page","link":"https:\/\/uniopt.co.jp\/en\/catalog\/birefringence\/sbr\/sbr-02\/","title":{"rendered":"SBR-02"},"content":{"rendered":"<p><!--:ja--><\/p>\n<hr \/>\n<ol>\n<li>Overview<br \/>\nThe SBR-02 is based on the rotational polarizer method used in ellipsometers. The optical system is almost the same as that of the SBR-01, but by rotating the polarizer on the light source side, the birefringent phase difference and the principal axis orientation of the sample can be determined simultaneously. <a href=\"https:\/\/uniopt.co.jp\/wp-content\/uploads\/2014\/05\/SBR02.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-medium wp-image-403\" src=\"https:\/\/uniopt.co.jp\/wp-content\/uploads\/2014\/05\/SBR02-300x271.jpg\" alt=\"SBR02\" width=\"300\" height=\"271\" srcset=\"https:\/\/uniopt.co.jp\/wp-content\/uploads\/2014\/05\/SBR02-300x271.jpg 300w, https:\/\/uniopt.co.jp\/wp-content\/uploads\/2014\/05\/SBR02.jpg 354w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n<hr \/>\n<\/li>\n<li>Perfarmance \n<table id=\"tablepress-25\" class=\"tablepress tablepress-id-25 tbody-has-connected-cells\">\n<thead>\n<tr class=\"row-1\">\n\t<td class=\"column-1\"><\/td><th class=\"column-2\">Specification<\/th><th class=\"column-3\">Retardation<\/th><th class=\"column-4\">Azimuth of axis<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr class=\"row-2\">\n\t<td rowspan=\"3\" class=\"column-1\">Measurement performance<\/td><td class=\"column-2\">Resolution<\/td><td class=\"column-3\">0.1 deg. (0.2 nm at 633 nm)<\/td><td class=\"column-4\">0.1 deg.<\/td>\n<\/tr>\n<tr class=\"row-3\">\n\t<td class=\"column-2\">Range<\/td><td class=\"column-3\">0 - 85 deg.<br \/>\n(0 - 150 nm at 633 nm)<\/td><td class=\"column-4\">\u00b1 90 deg.<\/td>\n<\/tr>\n<tr class=\"row-4\">\n\t<td class=\"column-2\">Measurement time<\/td><td colspan=\"2\" class=\"column-3\">Appx. 3 sec. \/ point<\/td>\n<\/tr>\n<tr class=\"row-5\">\n\t<td rowspan=\"2\" class=\"column-1\">Optical system<\/td><td class=\"column-2\">Principle of Measurement<\/td><td colspan=\"2\" class=\"column-3\">Rotating polarizer method<\/td>\n<\/tr>\n<tr class=\"row-6\">\n\t<td class=\"column-2\">Source<\/td><td colspan=\"2\" class=\"column-3\">He-Ne laser (\u03bb=632.8 nm)<br \/>\nOther wavelengths are available as an option.<\/td>\n<\/tr>\n<tr class=\"row-7\">\n\t<td class=\"column-1\">Sample stage<br \/>\n<\/td><td class=\"column-2\">Folding<\/td><td colspan=\"2\" class=\"column-3\">To be discussed separately(Standard scanning range : < 50 x 50 nm )<br \/>\nThe orientation of the main axis of the sample must be known (fixed orientation).<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<!-- #tablepress-25 from cache --><\/li>\n<\/ol>\n<hr \/>\n<p><!--:--><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Overview The SBR-02 is based on the rotational polarizer method used in ellipsometers. The optical system is a &hellip; <a href=\"https:\/\/uniopt.co.jp\/en\/catalog\/birefringence\/sbr\/sbr-02\/\">Continue reading <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"parent":2056,"menu_order":1,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_locale":"en_US","_original_post":"http:\/\/www.uniopt.co.jp\/?page_id=402","footnotes":""},"class_list":["post-2074","page","type-page","status-publish","hentry","en-US"],"aioseo_notices":[],"aioseo_head":"\n\t\t<!-- All in One SEO 4.9.9 - aioseo.com -->\n\t<meta name=\"description\" content=\"Overview The SBR-02 is based on the rotational polarize\" \/>\n\t<meta name=\"robots\" content=\"max-image-preview:large\" \/>\n\t<link rel=\"canonical\" href=\"https:\/\/uniopt.co.jp\/en\/catalog\/birefringence\/sbr\/sbr-02\/\" \/>\n\t<meta name=\"generator\" content=\"All in One SEO (AIOSEO) 4.9.9\" \/>\n\t\t<meta property=\"og:locale\" content=\"en_US\" \/>\n\t\t<meta 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