Abstract

Focussing and stigmation of the objective lens for high resolution STEM imaging is usually achieved by repeated reduced area scans of a given specimen area under manual control of the instrument. This method is particularly laborious since the scan times for images can be upwards of several seconds which subjects a specimen to unwanted electron beam exposure. Methods have been proposed to optimize STEM images such as the use of shadow images1 where a fixed beam pattern for a highly defocussed objective lens is observed. This method again requires a high beam dose in a given specimen area. Alternately, if a white noise object such as a carbon film is used, granular image features without any directionality are desired. In this case the eye must integrate over a large number of small image features. A better alternative is the use computer control to digitize images in real time and compute the power spectrum of an image could be employed. This would require a dedicated high speed computer system for a 1000 × 1000 display, but this latter method would have the advantage that only a single scan of image is required.

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