透過您的圖書館登入
IP:3.22.242.141
  • 期刊
  • OpenAccess
  • Ahead-of-Print

Cyclotron Emission from a Finite Thickness Neutralized Electron Beam

本文正式版本已出版,請見:10.6122/CJP.20140825B

並列摘要


Cyclotron emission from a neutralized, large orbit (LO) and finite thickness monochromatic electron beam in the presence of a right hand circularly polarized field of a plane electromagnetic wave is studied. Trajectories of N=50000 electrons whose gyration centers are randomly distributed within a circle of radius ∆, as well as their initial position that too are randomly located on their LOs, are followed. A restoring force caused by neutralizing ions is elective for electrons leaving the outer or the inner radii of the finite thickness beam. This force is introduced by a phenomenological potential well in the radial directions as was done previously for an infinitesimally thick beam [J. Plasma Phys., 73, 523{541, (2006)]. It is shown that for the beams having high density, the Cherenkov instability in the azimuthal direction (CIAD) with ω < Ω + k_zV_z causes the excitation of microwaves. With an increase in the beam thickness, the CIAD decreases and finally stops. Beyond this thickness, the cyclotron maser instability for ω > Ω + kzVz causes generation of microwaves.

並列關鍵字

無資料

延伸閱讀