Diode system on the basis of field emitter with semi-ellipsoid shape mathematical modeling

Author(s):  
Tatjana A. Maslova ◽  
Ekaterina M. Vinogradova
2011 ◽  
Vol 56 (9) ◽  
pp. 1219-1224 ◽  
Author(s):  
E. M. Vinogradova ◽  
N. V. Egorov

2020 ◽  
Vol 65 (4) ◽  
pp. 514-517
Author(s):  
E. M. Vinogradova ◽  
G. G. Doronin ◽  
N. V. Egorov

Author(s):  
Nickolay V. Egorov ◽  
◽  
Ekaterina M. Vinogradova ◽  

In this paper the mathematical modeling of the triode emission axially symmetric system on the basis of field emitter is considered. Emitter is an ellipsoid of revolution, anode is a confocal ellipsoidal surface of revolution. Modulator is a part of the ellipsoidal surface of revolution, confocal with the cathode and anode surfaces. The boundary-value problem for the Laplace's equation in the prolate spheroidal coordinates with the boundary conditions of the first kind is solved. The variable separation method is applied to calculate the axisymmetrical electrostatic potential distribution. The potential distribution is represented as the Legendre functions expansion. The expansion coefficients are the solution of the system of linear equations. All geometrical dimensions of the system are the parameters of the problem.


Vacuum ◽  
2016 ◽  
Vol 127 ◽  
pp. 45-50 ◽  
Author(s):  
E.M. Vinogradova ◽  
E.N. Egorov ◽  
D.S. Televnyy

Author(s):  
P.M. Mul ◽  
B.J.M. Bormans ◽  
L. Schaap

The first Field Emission Guns (FEG) on TEM/STEM instruments were introduced by Philips in 1977. In the past decade these EM400-series microscopes have been very successful, especially in analytical electron microscopy, where the high currents in small probes are particularly suitable. In High Resolution Electron Holography, the high coherence of the FEG has made it possible to approach atomic resolution.Most of these TEM/STEM systems are based on a cold field emitter (CFE). There are, however, a number of disadvantages to CFE’s, because of their very small emission region: the maximum current is limited (a strong disadvantage for high-resolution TEM imaging) and the emission is unstable, requiring special measures to reduce the strong FEG-induced noise. Thermal field emitters (TFE), i.e. a zirconiated field emitter source operating in the thermal or Schottky mode, have been shown to be a viable and attractive alternative to CFE’s. TFE’s have larger emission regions, providing much higher maximum currents, better stability, and reduced sensitivity to vacuum conditions as well as mechanical and electrical interferences.


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