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Ion Implantation and Synthesis of Materials - Studium

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15.2 Implanters Used in CMOS Processing 221Fig. 15.4. High energy beamline featuring an RF linac with 12 resonators. The ion source<strong>and</strong> analyzer magnets are on the left. The final energy magnet is on the rightdouble or triple charge states in a second charge exchange cell. Typical beam sizes<strong>and</strong> overall beamline length are comparable to the linac-based beamline.15.2.2 Other SubsystemsThe effective generation <strong>and</strong> transport <strong>of</strong> ion beams is the raison d’etre <strong>of</strong> ionimplanters, but working machines in wafer factories require a variety <strong>of</strong> othertechnologies.Wafer H<strong>and</strong>lingBecause ion implanters are high-throughput, high-vacuum systems, waferh<strong>and</strong>ling is rather unique <strong>and</strong> has been an area <strong>of</strong> proprietary technologydevelopment. Mechanical throughput has been on the order <strong>of</strong> 200 wafers per hour(wph) for many years, <strong>and</strong> recently throughput has increased to more than300 wph on new machines. Complex robotics are needed to automatically removewafers from cassettes or pods (in the case <strong>of</strong> 300 mm), orient them to ensurecorrect twist angle, transfer them to high vacuum (usually through a load-lockmechanism) <strong>and</strong> then to a spinning disk or electrostatic platen for implantation.Parallel operations minimize wafer-h<strong>and</strong>ling overhead in order to increase thefraction <strong>of</strong> time spent implanting.

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