TY - JOUR
T1 - X-mode electron cyclotron heating scenarios beyond the cut-off density
AU - Buermans, Johan
AU - Crombé, K.
AU - Dittrich, L.
AU - Goriaev, A.
AU - Kovtun, Yu
AU - Möller, S.
AU - López-Rodríguez, D.
AU - Petersson, P.
AU - Verstraeten, M.
AU - Wauters, T.
N1 - Publisher Copyright:
© 2023 Author(s).
PY - 2023/8/18
Y1 - 2023/8/18
N2 - Electron Cyclotron Heating (ECH) at the fundamental resonance in X-mode is limited by a low cut-off density. Electromagnetic waves cannot propagate in the region between this cut-off and the Upper Hybrid Resonance (UHR) and cannot reach the Electron Cyclotron Resonance (ECR) position. Higher harmonic heating is hence preferred in nowadays ECH plasma heating scenarios to overcome this problem. However, if this evanescent region is small compared to the wavelength of the waves, additional power deposition mechanisms can occur to increase the plasma density. This includes collisional losses in the evanescent region, tunneling of the X-wave with resonant coupling at the ECR, and conversion to the Electron Bernstein Wave (EBW) with resonant coupling. Several ECH plasma production experiments were performed on the TOMAS device with simple toroidal magnetic field to identify these additional heating regimes and to study the influence of the heating power on the ECH plasma parameters and the power deposition. Density and temperature profiles were measured with Langmuir Probes. Measurements of the forwarded and reflected power allow to estimate the coupling efficiency. The results help to understand ECH plasma production for tokamak plasma breakdown assistance and Electron Cyclotron Wall Conditioning (ECWC).
AB - Electron Cyclotron Heating (ECH) at the fundamental resonance in X-mode is limited by a low cut-off density. Electromagnetic waves cannot propagate in the region between this cut-off and the Upper Hybrid Resonance (UHR) and cannot reach the Electron Cyclotron Resonance (ECR) position. Higher harmonic heating is hence preferred in nowadays ECH plasma heating scenarios to overcome this problem. However, if this evanescent region is small compared to the wavelength of the waves, additional power deposition mechanisms can occur to increase the plasma density. This includes collisional losses in the evanescent region, tunneling of the X-wave with resonant coupling at the ECR, and conversion to the Electron Bernstein Wave (EBW) with resonant coupling. Several ECH plasma production experiments were performed on the TOMAS device with simple toroidal magnetic field to identify these additional heating regimes and to study the influence of the heating power on the ECH plasma parameters and the power deposition. Density and temperature profiles were measured with Langmuir Probes. Measurements of the forwarded and reflected power allow to estimate the coupling efficiency. The results help to understand ECH plasma production for tokamak plasma breakdown assistance and Electron Cyclotron Wall Conditioning (ECWC).
UR - http://www.scopus.com/inward/record.url?scp=85177023168&partnerID=8YFLogxK
U2 - 10.1063/5.0162523
DO - 10.1063/5.0162523
M3 - Conference article
AN - SCOPUS:85177023168
SN - 0094-243X
VL - 2984
JO - AIP Conference Proceedings
JF - AIP Conference Proceedings
IS - 1
M1 - 110003
T2 - 24th Topical Conference on Radio-frequency Power in Plasmas
Y2 - 26 September 2022 through 28 September 2022
ER -