B. N. A. Lamborn
Abstract
The relativistic Vlasov dispersion relation is used to find the critical density ${n}_{c}=\frac{3{{B}_{0}}^{2}\ensuremath{\kappa}T}{8\ensuremath{\pi}{m}^{2}{c}^{4}}$ below which the extraordinary wave can propagate freely across a mirror-field plasma into the cyclotron-resonance region.
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The relativistic Vlasov dispersion relation is used to find the critical density ${n}_{c}=\frac{3{{B}_{0}}^{2}\ensuremath{\kappa}T}{8\ensuremath{\pi}{m}^{2}{c}^{4}}$ below which the extraordinary wave can propagate freely across a mirror-field plasma into the cyclotron-resonance region.
Key concepts: Cyclotron, Plasma, Physics, Transmission (telecommunications), Atomic physics, Waves in plasmas, Nuclear physics, Telecommunications