scholarly journals Expected yields of Ta181(e,e′)Ta*181 in the multi-keV range with a plasma-cathode electron beam

2022 ◽  
Vol 105 (1) ◽  
Author(s):  
F. Gobet ◽  
A. Ya. Dzyublik ◽  
G. Gosselin ◽  
V. Méot ◽  
M. Versteegen
Keyword(s):  
2021 ◽  
Vol 118 (4) ◽  
pp. 044102
Author(s):  
F. Gobet ◽  
P. Barberet ◽  
L. Courtois ◽  
G. Deves ◽  
J. Gardelle ◽  
...  

Author(s):  
М.С. Воробьёв ◽  
П.В. Москвин ◽  
В.И. Шин ◽  
Н.Н. Коваль ◽  
К.Т. Ашурова ◽  
...  

The paper describes a method for a controlled change in the power of an electron beam during a pulse of submillisecond duration, using a source "SOLO" with a plasma cathode. The beam power is controlled by changing the amplitude of the beam current with a corresponding change in the concentration of the emission plasma. This control method allows generating submillisecond beams of variable power (up to 10 MW at a maximum rate of change of no more than 0.5 MW/µs), which can be used for processing various metallic materials in order to change the functional properties of their surface with the ability to control the rate of input of beam energy into the surface of these materials.


2019 ◽  
Vol 47 (8) ◽  
pp. 3579-3585 ◽  
Author(s):  
Andrey V. Kazakov ◽  
Alexander V. Medovnik ◽  
Efim M. Oks

2019 ◽  
Vol 1393 ◽  
pp. 012064
Author(s):  
M S Vorobyov ◽  
N N Koval ◽  
P V Moskvin ◽  
A D Teresov ◽  
S Yu Doroshkevich ◽  
...  

2019 ◽  
Vol 90 (2) ◽  
pp. 023302 ◽  
Author(s):  
I. Yu. Bakeev ◽  
A. S. Klimov ◽  
E. M. Oks ◽  
A. A. Zenin

2019 ◽  
Vol 1393 ◽  
pp. 012055 ◽  
Author(s):  
V I Shin ◽  
P V Moskvin ◽  
M S Vorobyov ◽  
V N Devyatkov ◽  
S Yu Doroshkevich

2019 ◽  
Vol 37 (2) ◽  
pp. 203-208 ◽  
Author(s):  
Aleksandr Klimov ◽  
Ilya Bakeev ◽  
Efim Oks ◽  
Aleksey Zenin

AbstractWe describe here the design, main parameters, and characteristics of a forevacuum-pressure plasma-cathode electron source based on a hollow-cathode discharge. The source generates a continuous focused electron beam with energy up to 30 keV and current up to 300 mA at a pressure of 10–50 Pa. The focused electron beam reaches a maximum power density of 106 W/cm2. The source utility has been demonstrated by its application for processing and cutting of ceramic.


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