Nordsieck’s equation for a quasi-stationary relativistic electron beam propagating in a dense and rarefied gas-plasma medium along an external magnetic field
Abstract:
An equation is derived for the envelope of a quasi-stationary relativistic electron beam propagating in a gas-plasma medium. It generalizes the well-known Nordsieck equation to the case of the presence of an external longitudinal magnetic field both under the beam transportation in an ohmic plasma and under ion focusing conditions. A formula for the rms radius of the beam at the stage of intense expansion with regard to a compensating ionic background, multiple scattering, and an external longitudinal magnetic field is found.