Onset and Saturation of the Electric-Field Amplitude in Transit-Time Tubes

TLDR: In this paper, it was shown that the analytic expressions for the self-excitation condition and for saturation of the wave growth found on the basis of a 1-D circuit model are in excellent agreement with a full scale 2 frac12 -D particle-in-cell simulation.

Abstract: The monotron lumped equivalent circuit can be thought of as consisting of a physical tuned circuit connected to a resistor of negative resistance. For transit times near (N+1/4)T, where N is an integer and T the oscillation period, electron bunches are formed and upon reaching the cavity's end plate in a decelerating phase of the RF field the bunches transfer energy to the cavity. The relation between current and voltage is set by the beam conductance, which is always non linear, so that for one amplitude will there be a given ratio between current and voltage. From the equation of motion of the beam electrons interacting with the RF fields, such relation - the electronic beam nonlinear conductance G(V2) - is found by expanding the conversion efficiency up to the tenth power of the RF voltage amplitude. Then using G(V2) in the energy balance equation (relating the RF power losses in the cavity and the microwave power radiated by the electron beam) we arrive at the van der Pol's equation, just describing the non linear growth and the stationary generation of the electromagnetic mode operating in the cavity driven by the externally injected beam. It is shown that the analytic expressions for the self-excitation condition and for the saturation of the wave growth found on the basis of a 1-D circuit model are in excellent agreement with a full scale 2 frac12 -D particle-in-cell simulation.