Abstract
Test particle evaluation of the diffusion coefficient in the presence of magnetic field fluctuations and binary collisions is presented. Chaotic magnetic field lines originate from resonant magnetic perturbations (RMPs). To lowest order, charged particles follow magnetic field lines. Drifts and interaction (collisions) with other particles decorrelate particles from the magnetic field lines. We model the binary collision process by a constant collision frequency. The magnetic field configuration including perturbations on the integrable Hamiltonian part is such that the single particle motion can be followed by a collisional version of a Chirikov-Taylor (standard) map. Frequent collisions are allowed for. Scaling of the diffusion beyond the quasilinear and subdiffusive behaviour is investigated in dependence on the strength of the magnetic perturbations and the collision frequency. The appearance of the so called Rechester-Rosenbluth regime is verified. It is further shown that the so called Kadomtsev-Pogutse diffusion coefficient is the strong collisional limit of the Rechester-Rosenbluth formula. The theoretical estimates are supplemented by numerical simulations.
Original language | English |
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Article number | 023114 |
Journal | Chaos |
Volume | 22 |
Issue number | 2 |
DOIs | |
State | Published - Apr 4 2012 |
Externally published | Yes |
Funding
The authors acknowledge discussions with Adriane Schelin, Berhard Unterberg, and Yunfeng Liang. The work was supported by DFG under SP 229/1-1 and FZ Jülich.
Funders | Funder number |
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Deutsche Forschungsgemeinschaft | SP 229/1-1 |