Ion-Focused Propagation of Relativistic Electron Beam in the Self-Generated Plasma in the Atmosphere

2022 ◽  
Author(s):  
Hao Jian-Hong ◽  
Xue Bi-Xi ◽  
Zhao Qiang ◽  
Zhang Fang ◽  
Fan Jie-Qing ◽  
...  

Abstract It is known that ion-focused regime can effectively suppress the expansion of relativistic electron beam (REB). By using particle in cell-Monte Carlo collision (PIC-MCC) method, the propagation of REBs in neutral gas is numerically investigated. The numerical results demonstrate that the beam body is charge neutralization and a stable IFR can be established. As a result, the beam transverse dimensions and longitudinal velocities keep close to the initial parameters. We also calculated the charge and current neutralization factors of REBs. Combined with envelope equations, we obtained the variations of beam envelopes, which agree well with the PIC simulations. However, both the energy loss and instabilities of REBs may lead to a low transport efficiency during long-range propagation. It has been proved that decreasing the initial pulse length of REBs can avoid the influence of electron avalanche. Using parts of REB pulses to build a long-distance IFR in advance can improve the beam quality of subsequent pulses. Further, a long-distance IFR may contribute to the implementation of long-range propagation of REBs in the space environment.

1976 ◽  
Vol 16 (1) ◽  
pp. 81-94 ◽  
Author(s):  
F. Winterberg

Because of the technical difficulties associated with the production of ultrashort beam pulses, the efforts to release energy from thermonuclear microexplosions are mainly directed at present towards confinement in a high-Z material solid wall, as in the original proposal by the author for relativistic electron beam induced fusion. The most common approach today is by the implosion of a solid high-Z material shell, for example, with an intense relativistic electron beam. We will show that better utilization of the beam energy may be possible with beam bombardment of a curved concave wall, setting off a shock wave which can be focused precisely onto the thermonuclear target. In addition, by a proper variation of the atomic weight and density in the layer of the wall material to be ablated by the energy deposition of the beam, the pulse length of the shock wave can be made substantially shorter than the pulse length of the beam.


2009 ◽  
Vol 80 (1) ◽  
Author(s):  
Anupam Karmakar ◽  
Naveen Kumar ◽  
Alexander Pukhov ◽  
O. Polomarov ◽  
Gennady Shvets

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