ABSTRACT:
Recent experimental confirmation of various mechanisms of fastion transport by instabilities in magneticallyconfined plasma is presented. Energy transfer de E is the perturbed electric field ωpends on v · E, where is the fastion velocity, produced by the instability, and the integral is over the orbit. For instabilities that do not coincide with frequencies of orbital motion (nonresonant instabilities), the large orbits of fast ions reduce transport via phaseaveraging of the electric field. Drift waves with small spatial structure cause less transport than drift waves with large structure, and coherent waves cause less transport than turbulent waves. For a sawtooth instability with a large, transient electric field, trapped particles with large drift orbits that decouple the ions from flux surfaces suffer less transport than passing particles. Resonant instabilities are qualitatively different. The standard resonance condition for modes with frequencies ω ωci is = nωζ + pωθ. Here ci is the cyclotron frequency, n is the toroidal mode number of the instability, p is an integer, and ωζ and ωθ are the toroidal and poloidal frequencies of the orbital motion. Coherent resonant losses occur when Alfv´en waves push fast ions onto loss orbits. A large fraction of the fastion population is expelled via coherent losses when large global modes maintains the resonance condition across much of the plasma. Multiple resonances often produce diffusive transport. Many smallamplitude Alfv´en eigenmodes cause diffusive flattening of the fastion profile. For large mode amplitudes, other resonant transport mechanisms become operative. Above a certain threshold, an avalanche of different Alfv´en waves can be excited, causing substantial transport. Large amplitude waves can nonlinearly excite new resonances at harmonics and subharmonics of the orbital frequencies, as recently observed for energeticparticle driven geodesic acoustic modes.