K. Toi , M. Takechi 1, S. Takagi 1,
G. Matsunaga 1, M. Isobe , T. Kondo 2,
M. Sasao , D. S. Darrow 3, K. Ohkuni 1,
S. Ohdachi , R. Akiyama , A. Fujisawa , M. Gotoh ,
H. Idei , K. Ida , H. Iguchi , S. Kado , M. Kojima ,
S. Kubo , S. Lee , K. Matsuoka , T. Minami ,
S. Morita , N. Nikai 1, S. Nishimura , S. Okamura ,
M. Osakabe , A. Shimizu 1, Y. Shirai 2,
C. Takahashi , K. Tanaka , T. Watari , Y. Yoshimura
National Institute for Fusion Science, Toki-shi 509-5292, Japan
1 Dep. Energy Eng. Science, Nagoya Univ., Nagoya 464-8603, Japan
2 The Graduate Univ. for Advanced Studies, Toki-shi, 509-5292, Japan
3 Princeton Plasma Physics Laboratory, Princeton, N.J., U.S.A.
Abstract
In the CHS heliotron /torsatron , fishbone instabilities(FBs)
and toroidal Alfven eigenmodes(TAEs) are observed for the first time, in NBI
heated plasmas where small beam driven current is induced. Pulsed increase in
energetic ion loss flux is detected by an escaping ion probe during the
m=3/n=2 FBs(m,n: poloidal and toroidal mode numbers). The sawtooth crash is
often induced by the m=2/n=1 FBs. The current driven internal kink mode and
pressure driven interchange modes are thought to be relevant MHD instabilities
to FBs. TAEs with n=1 and n=2 are identified, and localized near the plasma
core region where fairly low magnetic shear would be realized by the small net
plasma current. So far, the observed TAEs do not lead to enhanced loss of
energetic ions because of low magnetic fluctuation level.
IAEA 1999