From onedimensional fields to Vlasov equilibria: theory and application of Hermite polynomials
Abstract
We consider the theory and application of a solution method for the inverse problem in collisionless equilibria, namely that of calculating a VlasovMaxwell equilibrium for a given macroscopic (fluid) equilibrium. Using Jeans' theorem, the equilibrium distribution functions are expressed as functions of the constants of motion, in the form of a Maxwellian multiplied by an unknown function of the canonical momenta. In this case it is possible to reduce the inverse problem to inverting Weierstrass transforms, which we achieve by using expansions over Hermite polynomials. A sufficient condition on the pressure tensor is found which guarantees the convergence and the boundedness of the candidate solution, when satisfied. This condition is obtained by elementary means, and it is clear how to put it into practice. We also argue that for a given pressure tensor for which our method applies, there always exists a positive distribution function solution for a sufficiently magnetised plasma. Illustrative examples of the use of this method with both forcefree and nonforcefree macroscopic equilibria are presented, including the full verification of a recently derived distribution function for the forcefree Harris sheet (Allanson et al., Phys. Plasmas, vol. 22 (10), 2015, 102116). In the effort to model equilibria with lower values of the plasma β, solutions for the same macroscopic equilibrium in a new gauge are calculated, with numerical results presented for β_{pl}=0.05.
 Publication:

Journal of Plasma Physics
 Pub Date:
 June 2016
 DOI:
 10.1017/S0022377816000519
 arXiv:
 arXiv:1606.01661
 Bibcode:
 2016JPlPh..82c9006A
 Keywords:

 Physics  Plasma Physics
 EPrint:
 Published version is Open Access in Journal of Plasma Physics, 82, 03 (2016). arXiv admin note: substantial text overlap with arXiv:1508.07925