Discrete maps have been extensively used to model 2-dimensional chaotic transport in plasmas and fluids. Here we focus on area-preserving maps describing finite Larmor radius (FLR) effects on E × B chaotic transport in magnetized plasmas with zonal flows perturbed by electrostatic drift waves. FLR effects are included by gyro-averaging the Hamiltonians of the maps which, depending on the zonal flow profile, can have monotonic or non-monotonic frequencies. In the limit of zero Larmor radius, the monotonic frequency map reduces to the standard Chirikov-Taylor map, and, in the case of non-monotonic frequency, the map reduces to the standard nontwist map. We show that in both cases FLR leads to chaos suppression, changes in the stability of fixed points, and robustness of transport barriers. FLR effects are also responsible for changes in the phase space topology and zonal flow bifurcations. Dynamical systems methods based on recurrence time statistics are used to quantify the dependence on the Larmor radius of the threshold for the destruction of transport barriers. * Electronic address: jfonseca@if.usp.br † Electronic address: delcastillod@ornl.gov ‡ Electronic address: ibere@if.usp.br 1 arXiv:1409.3106v1 [physics.plasm-ph]

No abstract

A statistical study of finite Larmor radius (FLR) effects on transport driven by electrostatic driftwaves is presented. The study is based on a reduced discrete Hamiltonian dynamical system known as the gyro-averaged standard map (GSM). In this system, FLR effects are incorporated through the gyro-averaging of a simplified weak-turbulence model of electrostatic fluctuations. Formally, the GSM is a modified version of the standard map in which the perturbation amplitude, K 0 , becomes K 0 J 0 (ρ), where J 0 is the zeroth-order Bessel function andρ is the Larmor radius. Assuming a Maxwellian probability density function (pdf) forρ, we compute analytically and numerically the pdf and the cumulative distribution function of the effective drift-wave perturbation amplitude K 0 J 0 (ρ). Using these results we compute the probability of loss of confinement (i.e., global chaos), P c , and the probability of trapping in the main drift-wave resonance, P t . It is shown that P c provides an upper bound for the escape rate, and that P t provides a good estimate of the particle trapping rate. The analytical results are compared with direct numerical Monte-Carlo simulations of particle transport. * Electronic address:

No abstract