Electron Optics of an Electron-Beam Lithographic System

1977 ◽  
Vol 21 (6) ◽  
pp. 514-521 ◽  
Author(s):  
J. L. Mauer ◽  
H. C. Pfeiffer ◽  
W. Stickel
Author(s):  
T. Mulvey

Research into the properties of cathode rays started in the 1850's when Geissler found out how to make vacuum tight gas-metal seals. It was soon discovered how to deflect the beam and concentrate it into a relatively small spot by means of a long magnetic solenoid, the theory of which was well established. Gabor's short concentrating coil complete with iron outer-shroud, shown in Fig 1., was introduced into a high voltage oscillograph in the period 1924-1926. It worked well but did not fit into the classical theoretical framework. The correct explanation of the action of a short coil in focussing an electron beam and its analogy with the focussing effect of the “burning glass” was first given by Hans Busoh in 1926. Busch left several questions open concerning the optical analogy and in 1928 Max Knoll and his student Ernst Ruska began in Berlin the first systematic investigation in “electron-optics”, with the aid of the electron-optical bench shown in Fig 2.


2017 ◽  
Author(s):  
Akira Kojima ◽  
Naokatsu Ikegami ◽  
Hiroshi Miyaguchi ◽  
Takashi Yoshida ◽  
Ryutaro Suda ◽  
...  

Microscopy ◽  
2021 ◽  
Author(s):  
Te Shi ◽  
Shikai Liu ◽  
H Tian ◽  
Z J Ding

Abstract In transmission electron microscope (TEM), both the amplitude and the phase of electron beam change when electrons traverse a specimen. The amplitude is easily obtained by the square root of the intensity of a TEM image, while the phase affects defocused images. In order to obtain the phase map and verify the theoretical model of the interaction between electron beam and specimen, a lot of simulations have to be performed by researchers. In this work, we have simulated defocus images of a SiC nanowire in TEM with the method of electron optics. Mean inner potential and charge distribution on the nanowire have been considered in the simulation. Besides, due to electron scattering, coherence loss of the electron beam has been introduced. A dynamic process with Bayesian optimization was used in the simulation. With the infocus image as input and by adjusting fitting parameters, the defocus image is determined with a reasonable charge distribution. The calculated defocus images are in a good agreement with the experimental ones. Here, we present a complete solution and verification method for solving nanoscale charge distribution in TEM.


1968 ◽  
Vol 15 (6) ◽  
pp. 430-431 ◽  
Author(s):  
K.T. Rogers ◽  
J. Kelly ◽  
D.L. Cogswell ◽  
E.R. Westerberg

1967 ◽  
Author(s):  
K.T. Rogers ◽  
J. Kelly ◽  
D.L. Cogswell ◽  
E.R. Westerberg

Sign in / Sign up

Export Citation Format

Share Document