Abstract
Beam-ion losses induced by fast-ion-driven toroidal Alfvén eigenmodes (TAE) were measured with a scintillator-based lost fast-ion probe (SLIP) in the large helical device (LHD). The SLIP gave simultaneously the energy E and the pitch angle χ = arccos(υ ///υ) distribution of the lost fast ions. The loss fluxes were investigated for three typical magnetic configurations of R ax-vac = 3.60 m, 3.75 m, and 3.90 m, where R ax-vac is the magnetic axis position of the vacuum field. Dominant losses induced by TAEs in these three configurations were observed in the E/χ regions of 50∼190 keV/40°, 40∼170 keV/25°, and 30∼190 keV/30°, respectively. Lost-ion fluxes induced by TAEs depend clearly on the amplitude of TAE magnetic fluctuations, R ax-vac and the toroidal field strength B t. The increment of the loss fluxes has the dependence of (b TAE/B t) s. The power s increases from s = 1 to 3 with the increase of the magnetic axis position in finite beta plasmas.
| Original language | English |
|---|---|
| Pages (from-to) | 269-272 |
| Number of pages | 4 |
| Journal | Plasma Science and Technology |
| Volume | 14 |
| Issue number | 4 |
| DOIs | |
| State | Published - Apr 2012 |
Keywords
- fast ion loss
- the large helical device
- toroidal Alfvén eigenmode
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