Backscattering of gyrotron radiation and short-wavelength turbulence during electron cyclotron resonance plasma heating in the L-2M stellarator

• Published in: Plasma physics reports Vol. 39; no. 6; pp. 444 - 455
• Main Authors: Batanov, G. M., Borzosekov, V. D., Kovrizhnykh, L. M., Kolik, L. V., Konchekov, E. M., Malakhov, D. V., Petrov, A. E., Sarksyan, K. A., Skvortsova, N. N., Stepakhin, V. D., Kharchev, N. K.
• Format: Journal Article
• Language: English
• Published: Boston Springer US 01.06.2013
• Subjects: 70 PLASMA PHYSICS AND FUSION TECHNOLOGY; Atomic; BACKSCATTERING; ECR HEATING; ELECTRON CYCLOTRON-RESONANCE; FLUCTUATIONS; GYROFREQUENCY; HEAT FLUX; INTERFERENCE; Molecular; NEOCLASSICAL TRANSPORT THEORY; Optical and Plasma Physics; Physics; Physics and Astronomy; PLASMA SIMULATION; Stellarators; TURBULENCE; WAVELENGTHS; Microwave Beam; Plasma Physic Report; Scattered Signal; Electron Cyclotron Resonance Heating; Electron Cyclotron Resonance
• ISSN: 1063-780X; 1562-6938
• DOI: 10.1134/S1063780X13060019

Backscattering of gyrotron radiation (θ = π) by short-wavelength density fluctuations ( k ⊥ = 30 cm −1 ) in the plasma of the L-2M stellarator was studied under conditions of electron cyclotron resonance (ECR) plasma heating at the second harmonic of the electron gyrofrequency (75 GHz). The scattering of the O-wave emerging due to the splitting of the linearly polarized gyrotron radiation into the X- and O-waves was analyzed. The signal obtained after homodyne detection of scattered radiation is a result of interference of the reference signal, the quasi-steady component, and the fast oscillating component. The coefficients of reflection of the quasi-steady component, R = 2 ( Y ), and fast oscillating component, R ∼ 2 ( Y ), of scattered radiation are estimated. The growth of the R ∼ 2 ( Y ) coefficient from 3.7 × 10 −4 to 5.2 × 10 −4 with increasing ECR heating power from 190 to 430 kW is found to correlate with the decrease in the energy lifetime from 1.9 to 1.46 ms. The relative density of short-wavelength fluctuations is estimated to be 〈 n ∼ 2 〉/〈 n e 2 〉 = 3 × 10 −7 . It is shown that the frequencies of short-wavelength fluctuations are in the range 10–150 kHz. The recorded short-wavelength fluctuations can be interpreted as structural turbulence, the energy of which comprises ∼10% of the total fluctuations energy. Simulations of transport processes show that neoclassical heat fluxes are much smaller than anomalous ones. It is suggested that short-wavelength turbulence plays a decisive role in the anomalous heat transport.