### Session J5: Invited Session: The Dynamics of Waves and Energetic Particles: Observations

1:30 PM–3:18 PM, Sunday, April 1, 2012
Room: International Ballroom South

Chair: Donald Spong, Oak Ridge National Laboratory

Abstract ID: BAPS.2012.APR.J5.2

### Abstract: J5.00002 : Energetic Particle Transport by Instabilities in Fusion Plasmas

2:06 PM–2:42 PM

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#### Author:

William Heidbrink
(UC Irvine)

Recent experimental confirmation of various mechanisms of fast-ion transport by instabilities in magnetically-confined plasma is presented. Energy transfer depends on $\oint \vec v\cdot\vec E$, where $\vec v$ is the fast-ion velocity, $\vec E$ is the perturbed electric field produced by the instability, and the integral is over the orbit. For instabilities that do {\it not} coincide with frequencies of orbital motion (non-resonant instabilities), the large orbits of fast ions reduce transport via phase-averaging 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 $\omega\ll\omega_{ci}$ is $\omega=n\omega_\zeta+p\omega_\theta$. Here $\omega_{ci}$ is the cyclotron frequency, $n$ is the toroidal mode number of the instability, $p$ is an integer, and $\omega_\zeta$ and $\omega_\theta$ 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 fast-ion 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 small-amplitude Alfv\'en eigenmodes cause diffusive flattening of the fast-ion 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 energetic-particle driven geodesic acoustic modes.

To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2012.APR.J5.2