{ "id": "1209.4289", "version": "v1", "published": "2012-09-19T15:57:06.000Z", "updated": "2012-09-19T15:57:06.000Z", "title": "Transition to chaos in magnetized, weakly coupled plasmas", "authors": [ "Andrea Carati", "Francesco Benfenati", "Alberto Maiocchi", "Luigi Galgani", "Matteo Zuin" ], "comment": "4 pages, 4 Figures. Submitted to PRL", "categories": [ "cond-mat.stat-mech", "physics.plasm-ph" ], "abstract": "We report the results of numerical simulations for a model of a one component plasma (a system of N point electrons with mutual Coulomb interactions) in a uniform stationary magnetic field. We take N up to 512, with periodic boundary conditions, and macroscopic parameters corresponding to the weak coupling regime, with a coupling parameter \\Gamma=1/64. We find that a transition from order to chaos takes place when the density is increased or the field decreased so that the ratio \\omega_p/\\omega_c between plasma and cyclotron frequencies becomes of order 1 (or equivalently the ratio r_L/\\lambda_D between Larmor radius and Debye length becomes of order 1). The result is in agreement with the theoretical prediction obtained in [1], on the basis of an old estimate of Iglesias, Lebowitz and MacGowan [2] for the intensity of the electric field acting on one electron and due to all the other ones. A comparison can be made with the threshold obtained from kinetic theory arguments, which corresponds to the condition \\nu_{ee}/\\omega_c=1, where \\nu_{ee} is the electron collision frequency. The latter threshold has a completely different dependence on the physical parameters and, for \\Gamma=1/64, gives a critical value of \\omega_p about 80 times larger.", "revisions": [ { "version": "v1", "updated": "2012-09-19T15:57:06.000Z" } ], "analyses": { "keywords": [ "weakly coupled plasmas", "transition", "uniform stationary magnetic field", "electron collision frequency", "mutual coulomb interactions" ], "note": { "typesetting": "TeX", "pages": 4, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2012arXiv1209.4289C" } } }