Abstract
Results are presented from experimental studies of the influence of the stellarator magnetic field structure on the plasma behavior in electron-cyclotron resonance regimes with a high heating power per electron. The magnetic field structure was changed by varying the induction current I p from −14 to +14 kA. The plasma electrons were heated at the second harmonic of the electron gyrofrequency by an X-mode microwave beam with a power of P ∼ 200 kW, the average plasma density being in the range n e = (0.5–2) × 1013 cm−3. At I p = 0, the rotational transform varies from \(\rlap{--} \iota \)(0) = 0.2 on the magnetic axis to 0.8 at the plasma boundary. At a positive current of I p = 13.5 kA, the rotational transform was \(\rlap{--} \iota \)(0) = 0.8 on the axis and \(\rlap{--} \iota \)(a p) = 0.9 at the plasma boundary. Experiments with a positive current have shown that the radiative temperature first increases with current. When the current increases to I p = 11–14 kA, strong modulation appears in the electron cyclotron emission signals received from all the plasma radii, the emission spectrum changes, and the emission intensity decreases. At a negative current of I p = −(6.5–13.5) kA, the rotational transform vanishes at r/a p = 0.4–0.6. In this regime, the number of suprathermal electrons is reduced substantially and the emission intensity decreases at both low and high plasma densities.
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Original Russian Text © D.K. Akulina, G.A. Gladkov, S.E. Grebenshchikov, O.I. Fedyanin, S.V. Shchepetov, 2006, published in Fizika Plazmy, 2006, Vol. 32, No. 6, pp. 502–516.
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Akulina, D.K., Gladkov, G.A., Grebenshchikov, S.E. et al. Effect of the magnetic field structure on the intensity of electron cyclotron emission from the plasma of the L-2M stellarator. Plasma Phys. Rep. 32, 461–474 (2006). https://doi.org/10.1134/S1063780X0606002X
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DOI: https://doi.org/10.1134/S1063780X0606002X