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Magnetohydrodynamic behaviour during core transport barrier experiments with ion Bernstein wave heating in PBX-M: IIn=m- 1 andn=mmodes

Authors :
B. LeBlanc
S. H. Batha
S. D. Pinches
A. Post-Zwicker
M.S. Chance
Paul P. Woskov
R.C. Isler
M. Ono
S. Kaye
R. Kaita
H. Takahashi
J. Manickam
A.C. England
S. Sesnic
Fred Levinton
S. von Goeler
J.L. Dunlap
S. C. Luckhardt
H. Kugel
T. Seki
W. Tighe
E. de la Luna
J. Sanchez Sanz
Stephen E. Jones
A. Zolfaghari
Sibylle Günter
R. Bell
S. Paul
Jay Kesner
F. Paoletti
M. Okabayashi
S. Bernabei
N. Sauthoff
Source :
Nuclear Fusion. 38:861-884
Publication Year :
1998
Publisher :
IOP Publishing, 1998.

Abstract

Two new types of high frequency (HF) MHD mode activity are observed when a core transport barrier is formed during ion Bernstein wave (IBW) heating in PBX-M. These modes, localized in the core transport barrier, seem to be mainly responsible for the soft saturation in the strength of the core transport barrier. The two types of HF mode activity are determined by the presence or absence of a strong 1/1 mode. The n = m modes are observed with the 1/1 mode, while the n = m - 1 modes are seen when the 1/1 mode is absent. The m numbers of both of these modes vary between 4 and 13. They all seem to be coupled and rotate as a rigid body. The n = m - 1 modes seemed to be narrowly localized on their corresponding rational surface, i.e. q = m/(m - 1). The modes are ballooning-like, and their amplitudes increase with increasing β. Calculations with the CASTOR code show that the n = m - 1 modes are most probably pressure driven tearing modes, but the possibility of kinetic ballooning modes (KBMs) cannot be fully excluded. The n = m modes appear on or around the q = 1 surface, and are localized at the X point of the 1/1 mode island. The frequency offset of the n = m modes, which is too low for a TAE, is shown to be consistent with β-induced toroidal Alfven eigenmodes (BAEs).

Details

ISSN :
00295515
Volume :
38
Database :
OpenAIRE
Journal :
Nuclear Fusion
Accession number :
edsair.doi...........786ed1756024407fc43e397f9b67e69d
Full Text :
https://doi.org/10.1088/0029-5515/38/6/306