A proposed high‐gradient laser‐driven electron accelerator using crossed cylindrical laser focusing

1996 ◽  
Vol 69 (15) ◽  
pp. 2175-2177 ◽  
Author(s):  
Y. C. Huang ◽  
R. L. Byer
Keyword(s):  
Electron Accelerator ◽  
High Gradient ◽  
Laser Focusing

High-gradient electron accelerator powered by a relativisitic klystron

1989 ◽  
Vol 63 (22) ◽  
pp. 2472-2475 ◽  
Author(s):  
M. Allen ◽  
J. Boyd ◽  
R. Callin ◽  
H. Deruyter ◽  
K. Eppley ◽  
...  
Keyword(s):  
Electron Accelerator ◽  
High Gradient

High Gradient Two-Beam Electron Accelerator

2010 ◽  
Author(s):  
Y. Jiang ◽  
S. Yu. Kazakov ◽  
S. V. Kuzikov ◽  
J. L. Hirshfield ◽  
Steven H. Gold ◽  
...  
Keyword(s):  
Electron Accelerator ◽  
High Gradient ◽  
Beam Electron

High-Gradient Electron Accelerator Powered by a Relativistic Klystron

1990 ◽  
Vol 64 (19) ◽  
pp. 2337-2337
Author(s):  
M. A. Allen ◽  
J. K. Boyd ◽  
R. S. Callin ◽  
H. Deruyter ◽  
K. R. Eppley ◽  
...  
Keyword(s):  
Electron Accelerator ◽  
High Gradient ◽  
Relativistic Klystron

Optical Properties of HVEM Accelerators

1975 ◽  
Vol 33 ◽  
pp. 180-181
Author(s):  
A. Strojnik ◽  
J.W. Scholl ◽  
V. Bevc
Keyword(s):  
Optical Properties ◽  
Electron Accelerator ◽  
Systematic Investigation ◽  
Electron Source ◽  
High Brightness ◽  
The Past ◽  
Wide Range ◽  
Optical Behavior

The electron accelerator, as inserted between the electron source (injector) and the imaging column of the HVEM, is usually a strong lens and should be optimized in order to ensure high brightness over a wide range of accelerating voltages and illuminating conditions. This is especially true in the case of the STEM where the brightness directly determines the highest resolution attainable. In the past, the optical behavior of accelerators was usually determined for a particular configuration. During the development of the accelerator for the Arizona 1 MEV STEM, systematic investigation was made of the major optical properties for a variety of electrode configurations, number of stages N, accelerating voltages, 1 and 10 MEV, and a range of injection voltages ϕ0 = 1, 3, 10, 30, 100, 300 kV).

CONSTRUCTION AND TEST OF A CHANNELING-RADIATION SOURCE AT THE NEW DARMSTADT SUPERCONDUCTING ELECTRON ACCELERATOR

1987 ◽  
Vol 48 (C9) ◽  
pp. C9-95-C9-98
Author(s):  
W. LOTZ ◽  
H. GENZ ◽  
A. RICHTER ◽  
W. KNÜPFER ◽  
J. P.F. SELLSCHOP
Keyword(s):  
Radiation Source ◽  
Electron Accelerator ◽  
Channeling Radiation
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