{"id":145,"date":"2020-02-14T18:34:33","date_gmt":"2020-02-14T10:34:33","guid":{"rendered":"https:\/\/www.bihec.com\/beam-imaging\/?p=145"},"modified":"2020-02-14T18:34:33","modified_gmt":"2020-02-14T10:34:33","slug":"beam-imaging-%e7%a6%bb%e5%ad%90%e6%9d%9f%e5%81%8f%e8%bd%ac%e5%99%a8-quadrupole-qid-900","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\/","title":{"rendered":"Beam Imaging \u79bb\u5b50\u675f\u504f\u8f6c\u5668 Quadrupole QID-900"},"content":{"rendered":"

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