The Optinium Space-Charge-Controlled Focus of an Electron Beam

1952 ◽  
Vol 5 (3) ◽  
pp. 430 ◽  
Author(s):  
DL Hollway

The problem of apace-charge defocusing of circular electron beams is considered. and expressions for the condition of optimum focus are derived from the equations of the beam profile. It is shown that, over a wide range of spot radii, the optimum-focus expressions may be replaced by much simpler relationships suited to electron-beam design problems.

1982 ◽  
Vol 13 ◽  
Author(s):  
B. Ahmed ◽  
R.A. McMahon

ABSTRACTElectron beams can transfer energy very efficiently to semiconductors. Systems have been developed for rapid heating to temperature around 1000°C under a variety of conditions from adiabatic to isothermal. Pulsed, focused, line and synthesized shaped beams are used to obtain a wide range of thermal cycles. The following applications are described: the annealing of ion-implanted Si, particularly the activation of As implants and shallow implants (Rp<150Å), the annealing of Si and Se in GaAs, the e-beam processing of implanted silicon devices and the improvement of SOS substrate quality. Localized annealing by a computer controlled e-beam and the recrystallization of deposited films on insulators are also considered.


Author(s):  
C J Humphreys ◽  
T J Bullough ◽  
R W Devenish ◽  
D M Maher ◽  
P S Turner

It has recently been found that electron beams, of energy typically 100 keV, can damage a very wide range of solids, many of which are normally thought to be stable to electron irradiation. For example, metals, semiconductors and ceramics can all be damaged by electrons having energy less than that required for direct displacement damage. Radiation damage effects are particularly apparent when using intense electron beams from field emission guns in STEM's, TEM's and SEM's, but damage also occurs in materials thought to be stable when using electrons from LaB6, or heated W filaments. Considerable care must therefore be taken in microanalysis, etc, particularly when using field emission guns.If the incident electron beam is focussed to nanometre-scale diameter, then nanometre-scale surface and volume structures (e.g. indentations, holes and lines) can be produced in a variety of specimens. It is also possible to cut a specimen to a desired shape with nanometre precision and to remove surface steps from surfaces, leaving them atomically smooth.


1999 ◽  
Vol 17 (1) ◽  
pp. 1-13
Author(s):  
JAYASHREE PANICKER ◽  
Y. CHOYAL ◽  
K.P. MAHESHWARI ◽  
U. SHARMA

An analytical and numerical study of the stability of sheet electron beams in periodically cusped magnetic fields (PCM) is made. The beam has been considered as having edges with a prescribed density variation. In estimating the electrostatic fields, we have considered the density variation of both the edges along the width and thickness of the sheet beam. The conditions for beam focusing and beam matching are discussed.


Author(s):  
D. E. Speliotis

The interaction of electron beams with a large variety of materials for information storage has been the subject of numerous proposals and studies in the recent literature. The materials range from photographic to thermoplastic and magnetic, and the interactions with the electron beam for writing and reading the information utilize the energy, or the current, or even the magnetic field associated with the electron beam.


Author(s):  
Tamotsu Ohno

The energy distribution in an electron; beam from an electron gun provided with a biased Wehnelt cylinder was measured by a retarding potential analyser. All the measurements were carried out with a beam of small angular divergence (<3xl0-4 rad) to eliminate the apparent increase of energy width as pointed out by Ichinokawa.The cross section of the beam from a gun with a tungsten hairpin cathode varies as shown in Fig.1a with the bias voltage Vg. The central part of the beam was analysed. An example of the integral curve as well as the energy spectrum is shown in Fig.2. The integral width of the spectrum ΔEi varies with Vg as shown in Fig.1b The width ΔEi is smaller than the Maxwellian width near the cut-off. As |Vg| is decreased, ΔEi increases beyond the Maxwellian width, reaches a maximum and then decreases. Note that the cross section of the beam enlarges with decreasing |Vg|.


Author(s):  
Y. Kokubo ◽  
W. H. Hardy ◽  
J. Dance ◽  
K. Jones

A color coded digital image processing is accomplished by using JEM100CX TEM SCAN and ORTEC’s LSI-11 computer based multi-channel analyzer (EEDS-II-System III) for image analysis and display. Color coding of the recorded image enables enhanced visualization of the image using mathematical techniques such as compression, gray scale expansion, gamma-processing, filtering, etc., without subjecting the sample to further electron beam irradiation once images have been stored in the memory.The powerful combination between a scanning electron microscope and computer is starting to be widely used 1) - 4) for the purpose of image processing and particle analysis. Especially, in scanning electron microscopy it is possible to get all information resulting from the interactions between the electron beam and specimen materials, by using different detectors for signals such as secondary electron, backscattered electrons, elastic scattered electrons, inelastic scattered electrons, un-scattered electrons, X-rays, etc., each of which contains specific information arising from their physical origin, study of a wide range of effects becomes possible.


2020 ◽  
Author(s):  
Mohit Tyagi ◽  
P. S. Sarkar ◽  
R. S. Sengar ◽  
Ashwani Kumar ◽  
Jagannath ◽  
...  

Author(s):  
Nikolai Yu. Peskov ◽  
Petr V. Kalinin ◽  
Stanislav L. Sinitsky ◽  
Andrey V. Arzhannikov ◽  
Evgeny S. Sandalov ◽  
...  

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