Sensitive 4 mm Lecher Wire Interferometer for Electron Concentration Measurements in Low‐Density Plasmas

1967 ◽  
Vol 38 (11) ◽  
pp. 1631-1633 ◽  
Author(s):  
J. Polman
1977 ◽  
Vol 1 (4) ◽  
pp. 206-211 ◽  
Author(s):  
S.A. Self ◽  
F.O. Reigel ◽  
R.M. Clements ◽  
R.K. James

1975 ◽  
Vol 18 (8) ◽  
pp. 806-809
Author(s):  
V. V. Belikovich ◽  
E. A. Benediktov ◽  
L. V. Grishkevich ◽  
V. A. Ivanov

2009 ◽  
Vol 49 (7) ◽  
pp. 1006-1010
Author(s):  
L. A. Shchepkin ◽  
G. M. Kuznetsova ◽  
G. P. Kushnarenko ◽  
K. G. Ratovsky

1968 ◽  
Vol 73 (11) ◽  
pp. 3511-3535 ◽  
Author(s):  
W. J. Heikkila ◽  
N. Eaker ◽  
J. A. Fejer ◽  
K. R. Tipple ◽  
J. Hugill ◽  
...  

Author(s):  
P.J. Killingworth ◽  
M. Warren

Ultimate resolution in the scanning electron microscope is determined not only by the diameter of the incident electron beam, but by interaction of that beam with the specimen material. Generally, while minimum beam diameter diminishes with increasing voltage, due to the reduced effect of aberration component and magnetic interference, the excited volume within the sample increases with electron energy. Thus, for any given material and imaging signal, there is an optimum volt age to achieve best resolution.In the case of organic materials, which are in general of low density and electric ally non-conducting; and may in addition be susceptible to radiation and heat damage, the selection of correct operating parameters is extremely critical and is achiev ed by interative adjustment.


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