Control of velocities generated in a two—dimensional collisionless plasma with symmetry

Abstract
The Cauchy Problem for the relativistic Vlasov–Maxwell equations is studied in two dimensions. The Cauchy data E0, B0 of the fields, and the initial density f0 of the plasma, are assumed to be smooth and to decay at infinity, and are to satisfy the usual constraints. When this data is restricted to be cylindrically symmetric, the v –support of the plasma density is shown to be bounded on every bounded time interval. However, a shock could still presumably be formed at very large times.

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