The response of a finite relativistic beam-plasma system to small disturbances is analysed using the coupled Vlasov-Maxwell equations. It is shown that when |ω−kV0|2≫ωβ2, where ωβ is the betatron frequency and V0 the drift velocity of the beam, straight-line orbits are sufficiently accurate to describe the beam-particle trajectories. Dispersion relations are derived for a finite beam and for both infinite and finite plasma configurations. The effect of a finite but large beam radius is shown to increase the growth of the electrostatic instability.
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G. Dorman (1966) studied this question.
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