Nonsingular Integral Equation for Stability of a Bunched Beam

Astronomy and Astrophysics – Astrophysics

Scientific paper

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Scientific paper

The usual linearized Vlasov equation for longitudinal motion of a bunched beam leads to a singular integral equation, with singularity where the coherent frequency equals a single-particle frequency: ω=Ω(J). A discretization for numerical solution of the equation in this form is not justified. A simple transformation gives a system which can be approximated by a matrix equation, because the new integral operator A is compact. The bunch becomes unstable at the current I for which det(1-A(ω,I)) first has a zero on the real ω-axis. Here A is a nonlinear function of ω. The theory and a realistic example will be presented.

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