Experimental High Resolution Dark Field Electron Microscopy

Author(s):  
Larry Pierce ◽  
Peter R. Buseck

High resolution dark field (DF) images of the superstructures of the pyrrhotite (Fe1-xS) and bornite-digenite (Cu5FeS4-Cu9S5) series can be related to structure. Further, they provide more detail than bright field (BF) images. The same objective aperture size and stigmater settings were used for DF as for BF imaging; symmetrical arrangements of diffracted beams in the objective aperture were used. Images that can be related to structure were obtained at the defocus value giving the greatest image contrast, thereby enabling proper defocusing without requiring extensive through-focus series.For the minerals of interest, diffraction patterns consist of many superstructure reflections and a few subcell reflections. BF images contain primarily features of the superstructure, presumably because the subcell reflections fall far from the axis of the objective lens and thus are affected by spherical and chromatic aberrations and beam divergence. Likewise, DF images formed with a similar arrangement of beams as that in BF contain only features of superstructure, but with reverse contrast to BF.

Author(s):  
M. Isaacson ◽  
J. Langmore ◽  
J. Wall ◽  
A. V. Crewe

The effort to image biological molecules by high resolution (2-4 Å) dark field electron microscopy has stimulated interest in those factors Which influence image contrast. It is known that elastically scattered electrons can be used to obtain high resolution information about a specimen. On the other hand, most inelastically scattered electrons cannot contribute any high resolution information about the specimen since they are the result of a nonlocalized interaction of the incident electrons with the electrons in the specimen. Moreover, in the conventional transmission electron microscope (CTEM) without a chromatic aberration corrector or an energy filter between the specimen and recording plane, inelastically scattered electrons blur the image, due to the chromatic aberration of the objective lens. This has particular importance in biological electron microscopy, since the ratio of total inelastic to elastic scattering for carbon is 1.6.


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