{"id":324,"date":"2024-03-31T20:24:44","date_gmt":"2024-03-31T12:24:44","guid":{"rendered":"https:\/\/www.bihec.com\/beam-imaging\/?p=324"},"modified":"2024-03-31T20:24:44","modified_gmt":"2024-03-31T12:24:44","slug":"beam-imaging-%e7%a6%bb%e5%ad%90%e6%9d%9f%e5%81%8f%e8%bd%ac%e5%99%a8-quadrupole-qid-900-5","status":"publish","type":"post","link":"https:\/\/www.bihec.com\/beam-imaging\/beam-imaging-%e7%a6%bb%e5%ad%90%e6%9d%9f%e5%81%8f%e8%bd%ac%e5%99%a8-quadrupole-qid-900-5\/","title":{"rendered":"Beam Imaging \u79bb\u5b50\u675f\u504f\u8f6c\u5668 Quadrupole QID-900"},"content":{"rendered":"<p>The model QID-900 deflects the incoming positive or negatively charged ion beam at 90 degrees in a two-dimensional electrostatic quadrupole field*. The quadrupole field is set up using a combination circular electrode and shim electrodes to produce hyperbolic equipotentials. A set of entrance and exit einzel lens assemblies correct any 2-dimensional focusing of the ion beam through the quadrupole. Some possible applications for the model QID-900 include:<\/p>\n<ul>\n<li>Merged ion-laser beam experiments<\/li>\n<li>Merged ion-neutral beam experiments<\/li>\n<li>Multiple beam line switching<\/li>\n<li>Separation of ions from molecular\/atomic\/neutral beam particles<\/li>\n<li>Separation of ions from photons<\/li>\n<li>Cluster deposition and ion spectroscopy<\/li>\n<li>Deflection of ions at either 90, 180 or 270 degrees<\/li>\n<li>Energy Filter<\/li>\n<\/ul>\n<h2>Product Specifications<\/h2>\n<div class=\"content-div\">\n<p><a href=\"http:\/\/beamimaging.com\/wp-content\/uploads\/2016\/10\/quadtstw.jpg\"><img decoding=\"async\" loading=\"lazy\" class=\"wp-image-211 size-medium alignnone\" src=\"http:\/\/beamimaging.com\/wp-content\/uploads\/2016\/10\/quadtstw-300x192.jpg\" alt=\"Quad\" width=\"300\" height=\"192\" \/><\/a> \u00a0\u00a0 <a href=\"http:\/\/beamimaging.com\/wp-content\/uploads\/2016\/10\/quadtstj.jpg\"><img decoding=\"async\" loading=\"lazy\" class=\"alignnone size-medium wp-image-212\" src=\"http:\/\/beamimaging.com\/wp-content\/uploads\/2016\/10\/quadtstj-300x192.jpg\" alt=\"Quad\" width=\"300\" height=\"192\" \/><\/a><\/p>\n<\/div>\n<p>The picture above left shows a 1 keV H<sub>2<\/sub>O<sup>+<\/sup>\u00a0(left) and N<sub>2<\/sub><sup>+<\/sup>\u00a0ion beam profiles before they are deflected, and after being deflected 90-degrees (right) using the model QID-900-H. The viewing area is 19mm diameter. \u00a0A\u00a0model G-2 Ion Gun System\u00a0with\u00a0model E-2 controller\u00a0were used to generate the ion beams. The images were recorded using the model\u00a0<a href=\"https:\/\/www.bihec.com\/beam-imaging\/tag\/bos-18\/\" title=\"View all posts in BOS-18\" target=\"_blank\">BOS-18<\/a> beam observation system, with model BOS-18-OPT02-2122 CCD camera, and model IPS-1 image processing system.<\/p>\n<br><div class=\"tagcloud\"><a href=\"https:\/\/www.bihec.com\/beam-imaging\/tag\/beam-imaging\/\" class=\"tag-cloud-link tag-link-0 tag-link-position-1\" style=\"font-size: 20.472727272727pt;\" aria-label=\"Beam Imaging (95\u4e2a\u9879\u76ee)\">Beam Imaging<\/a>\n<a href=\"https:\/\/www.bihec.com\/beam-imaging\/tag\/beamimaging\/\" class=\"tag-cloud-link tag-link-1 tag-link-position-2\" style=\"font-size: 22pt;\" aria-label=\"BeamImaging (126\u4e2a\u9879\u76ee)\">BeamImaging<\/a>\n<a href=\"https:\/\/www.bihec.com\/beam-imaging\/tag\/bis-bos\/\" class=\"tag-cloud-link tag-link-2 tag-link-position-3\" style=\"font-size: 20.472727272727pt;\" aria-label=\"BIS-BOS (94\u4e2a\u9879\u76ee)\">BIS-BOS<\/a>\n<a href=\"https:\/\/www.bihec.com\/beam-imaging\/tag\/quadrupole-qid-900\/\" class=\"tag-cloud-link tag-link-3 tag-link-position-4\" style=\"font-size: 8pt;\" aria-label=\"Quadrupole QID-900 (9\u4e2a\u9879\u76ee)\">Quadrupole QID-900<\/a>\n<a href=\"https:\/\/www.bihec.com\/beam-imaging\/tag\/%e7%94%b5%e5%ad%90%e6%9d%9f%e8%a7%82%e5%af%9f%e7%b3%bb%e7%bb%9f\/\" class=\"tag-cloud-link tag-link-4 tag-link-position-5\" style=\"font-size: 19.709090909091pt;\" aria-label=\"\u7535\u5b50\u675f\u89c2\u5bdf\u7cfb\u7edf (83\u4e2a\u9879\u76ee)\">\u7535\u5b50\u675f\u89c2\u5bdf\u7cfb\u7edf<\/a>\n<a href=\"https:\/\/www.bihec.com\/beam-imaging\/tag\/%e7%9c%9f%e7%a9%ba%e7%b3%bb%e7%bb%9f\/\" class=\"tag-cloud-link tag-link-5 tag-link-position-6\" style=\"font-size: 19.581818181818pt;\" aria-label=\"\u771f\u7a7a\u7cfb\u7edf (80\u4e2a\u9879\u76ee)\">\u771f\u7a7a\u7cfb\u7edf<\/a>\n<a href=\"https:\/\/www.bihec.com\/beam-imaging\/tag\/%e7%9c%9f%e7%a9%ba%e8%85%94\/\" class=\"tag-cloud-link tag-link-6 tag-link-position-7\" style=\"font-size: 19.454545454545pt;\" aria-label=\"\u771f\u7a7a\u8154 (79\u4e2a\u9879\u76ee)\">\u771f\u7a7a\u8154<\/a>\n<a href=\"https:\/\/www.bihec.com\/beam-imaging\/tag\/%e7%a6%bb%e5%ad%90%e6%9d%9f%e5%81%8f%e8%bd%ac%e5%99%a8\/\" class=\"tag-cloud-link tag-link-7 tag-link-position-8\" style=\"font-size: 16.145454545455pt;\" aria-label=\"\u79bb\u5b50\u675f\u504f\u8f6c\u5668 (43\u4e2a\u9879\u76ee)\">\u79bb\u5b50\u675f\u504f\u8f6c\u5668<\/a>\n<a href=\"https:\/\/www.bihec.com\/beam-imaging\/tag\/%e7%a6%bb%e5%ad%90%e6%9d%9f%e6%b5%81%e5%87%8f%e9%80%9f%e5%99%a8\/\" class=\"tag-cloud-link tag-link-8 tag-link-position-9\" style=\"font-size: 16.781818181818pt;\" aria-label=\"\u79bb\u5b50\u675f\u6d41\u51cf\u901f\u5668 (48\u4e2a\u9879\u76ee)\">\u79bb\u5b50\u675f\u6d41\u51cf\u901f\u5668<\/a>\n<a href=\"https:\/\/www.bihec.com\/beam-imaging\/tag\/%e7%a6%bb%e5%ad%90%e6%ba%90\/\" class=\"tag-cloud-link tag-link-9 tag-link-position-10\" style=\"font-size: 17.163636363636pt;\" aria-label=\"\u79bb\u5b50\u6e90 (52\u4e2a\u9879\u76ee)\">\u79bb\u5b50\u6e90<\/a><\/div>","protected":false},"excerpt":{"rendered":"<p>The model QID-900 deflects the incoming positive or negatively charged ion beam at 90 degr <\/p>\n","protected":false},"author":19,"featured_media":146,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_vp_format_video_url":"","_vp_image_focal_point":[]},"categories":[1],"tags":[18,3,8,38,6,20,19,36,29,22],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v17.5 - 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