Electron in the field of a classical and a quantized plane wave traveling in the same direction

1974 ◽  
Vol 17 (7) ◽  
pp. 952-956
Author(s):  
V. G. Bagrov ◽  
D. M. Gitman ◽  
V. A. Kuchin
Keyword(s):  
Plane Wave ◽  
Quantized Plane Wave

Fermion with an anomalous moment in a quantized plane wave field

1974 ◽  
Vol 17 (6) ◽  
pp. 864-866
Author(s):  
V. G. Bagrov ◽  
P. V. Bozrikov ◽  
D. M. Gitman
Keyword(s):  
Plane Wave ◽  
Wave Field ◽  
Anomalous Moment ◽  
Quantized Plane Wave ◽  
Plane Wave Field

Theory and Errors in Stereo Electron Microscopy

1968 ◽  
Vol 26 ◽  
pp. 336-337
Author(s):  
J. M. Pankratz
Keyword(s):  
Electron Microscopy ◽  
Transmission Electron Microscopy ◽  
Plane Wave ◽  
Focal Length ◽  
Foil Thickness ◽  
Points Of Interest ◽  
Transmission Electron ◽  
Vertical Spacing ◽  
Illuminating System

It is often desirable in transmission electron microscopy to know the vertical spacing of points of interest within a specimen. However, in order to measure a stereo effect, one must have two pictures of the same area taken from different angles, and one must have also a formula for converting measured differences between corresponding points (parallax) into a height differential.Assume (a) that the impinging beam of electrons can be considered as a plane wave and (b) that the magnification is the same at the top and bottom of the specimen. The first assumption is good when the illuminating system is overfocused. The second assumption (the so-called “perspective error”) is good when the focal length is large (3 x 107Å) in relation to foil thickness (∼103 Å).

A hybrid Gaussian and plane wave density functional scheme

1997 ◽  
Vol 92 (3) ◽  
pp. 477-487 ◽  
Author(s):  
GERALD LIPPERT ◽  
JuRG HUTTER ◽  
MICHELE PARRINELLO
Keyword(s):  
Plane Wave ◽  
Density Functional ◽  
Functional Scheme
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