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Stationary Solutions of the Flat Vlasov-Poisson System

机译:平板Vlasov-Poisson系统的固定解决方案

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The stationary solutions are triples (f,., U) of three functions: the distribution function f = f (x, v), the potential U = U (x) and the local density. =. (x), x, v. R2, which are linked by the Vlasov-Poisson system. We prove the existence of wide classes of spherically symmetric stationary solutions with the property that. depends on | x| = r and f on the energy E := U (x) + v2 2. First we answer the question of which given functions. are the local density of a stationary solution (inverse problem). Our result is (up to technicalities) that every. = 0 which is strictly decreasing on an interval [ 0, R) and zero on its complement (R similar to 8) belongs to this class. Second, we ask: which given functions q induce distribution functions f of the form f = q (-E0 -E) (E0 similar to 0) of a stationary solution? (direct problem). This question is answered for many q which are positive for positive and vanish for negative arguments in an approximative and constructive way which is based on numerical methods.
机译:静止解决方案是三个功能的三元组(f,u):分布函数f = f(x,v),电位U = u(x)和局部密度。 =。 (x),x,v。r2,由Vlasov-Poisson系统联系在一起。我们证明了具有属性的广泛球体对称固定解决方案的存在。取决于| x |能量E:= u(x)+ v2 2.首先,我们回答给定函数的问题。是静止解决方案的局部密度(反问题)。我们的结果是(达到技术人员)。 = 0在其补充(类似于8)的间隔[0,r)和零时严格递减,属于此类。其次,我们问:给定的函数Q诱导形式的分布函数f = q(-e0 -e)(e0类似于0)的静止解决方案? (直接问题)。对于许多Q来回答这个问题,这对于积极的积极争论是积极的,并且以近似和建设性的方式基于数值方法。

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