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Modification of sawteeth by second harmonic electron-cyclotron heating in a tokamak

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Electron-cyclotron heating, using second harmonic waves launched from the low field side, has a strong effect on sawteeth in the DIII-D tokamak [Plasma Physics and Controlled Nuclear Fusion Research, 1986 (IAEA, Vienna, 1987), Vol. I, p. 159]. There are two distinct methods and mechanisms for sawtooth period extension. In the first case a factor of 6 increase in sawtooth period, compared to that during Ohmic heating, occurs with electron-cyclotron heating (ECH) localized near the q=1 surface. The sawtooth period increases faster than linearly with increasing ECH power. Qualitatively, there is agreement with sawtooth suppression models, although details of the accompanying m/n=1/1 oscillation appear inconsistent. The second case is a technique for complete sawtooth suppression in which impurities and off-axis heating broaden the current profile and drive q0>1. It appears that the temperature and the current and q profiles inside q=1 are determined by the magnetohydrodynamic activity, which is modified by ECH, and not by the ECH power deposition directly.
Title: Modification of sawteeth by second harmonic electron-cyclotron heating in a tokamak
Description:
Electron-cyclotron heating, using second harmonic waves launched from the low field side, has a strong effect on sawteeth in the DIII-D tokamak [Plasma Physics and Controlled Nuclear Fusion Research, 1986 (IAEA, Vienna, 1987), Vol.
I, p.
159].
There are two distinct methods and mechanisms for sawtooth period extension.
In the first case a factor of 6 increase in sawtooth period, compared to that during Ohmic heating, occurs with electron-cyclotron heating (ECH) localized near the q=1 surface.
The sawtooth period increases faster than linearly with increasing ECH power.
Qualitatively, there is agreement with sawtooth suppression models, although details of the accompanying m/n=1/1 oscillation appear inconsistent.
The second case is a technique for complete sawtooth suppression in which impurities and off-axis heating broaden the current profile and drive q0>1.
It appears that the temperature and the current and q profiles inside q=1 are determined by the magnetohydrodynamic activity, which is modified by ECH, and not by the ECH power deposition directly.

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