scholarly journals A simple method for energy calibration of keV incident electron beam using a contactless electrostatic voltmeter probe

2021 ◽  
Vol 92 (8) ◽  
pp. 083301
Author(s):  
M. Belhaj ◽  
S. Dadouch
Author(s):  
A.E. Curzon

The heating effect of an incident electron beam may cause a material to be radiation-sensitive. For example, the adsorption behaviour of inert gases on graphite observed in a transmission electron microscope depends critically on the temperature of the substrate. Early consideration of beam heating dealt with a circular film illuminated at the centre by an electron beam of circular cross-section. In practice, however, the film is often supported across a square aperture and is not centrally illuminated. It has recently been shown that the method of images may be used to solve the problem of the heating of a square film of thermal conductivity k by a beam whose cross-section is entirely within the film. This solution has the advantage that it applies regardless of where the incident electron beam strikes the film. The general solution involves an infinite sum over a two dimensional lattice of heat sources and sinks. Though the sum is readily evaluated by means of a computer, it is helpful to consider a particular limiting case which is readily understood in terms of three images and the main beam. This case is illustrated in Figure 1.


Vacuum ◽  
1976 ◽  
Vol 26 (10-11) ◽  
pp. 421
Author(s):  
J.P. Coad ◽  
M. Gettings ◽  
J.C. Rivière

2005 ◽  
Vol 76 ◽  
pp. S152
Author(s):  
B. De Smedt ◽  
N. Reynaert ◽  
F. Flachet ◽  
M. Coghe ◽  
L. Paelinck ◽  
...  

1964 ◽  
Vol 17 (1) ◽  
pp. 45
Author(s):  
V Metchnik

Experimental results are given for the measurements of the absolute intensity of characteristic Ka radiation from a thick copper target when the normal to the target is inclined to the incident electron beam at an angle (I equal to 20�, 30�, 40�, and 50�. These measurements cover a range of electron energies between 20 and 50 kV, and take�off angles q, ranging from 1� to 50�. A comparison is made with the emission at normal incidence. The copper Ka radiation was isolated by means of balanced nickel and iron filters, and the intensity mllasurements were made with a scintillation counter with NaI(TI) crystal


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