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10-15 May 2021
Nice, France
Europe/Vienna timezone
The Conference will be held virtually from 10-15 May 2021

High-performance ECRH at W7-X: Experience and Perspectives

13 May 2021, 14:00
4h 45m
Nice, France

Nice, France

Regular Poster Magnetic Fusion Experiments P6 Posters 6


Heinrich Laqua (Max-Planck-Institute for Plasma Physics, Greifswald, Germany)


W7-X is the first large fusion device where stationary reactor relevant densities have been achieved with electron heating only as it will be also the case for alpha particle heated fusion reactors. Employing the multi-pass ECRH scenario in the second harmonic O-mode (O2-ECRH), stationary (12 s) densities of up to 1.5 1020 m-3 had been achieved with hydrogen gas fueling. This scenario also made the stationary divertor detachment possible [1]. With a strongly reduced power load at the divertor tiles, detachment is a candidate for particle and power exhaust in fusion reactors. Even though electrons have been heated primarily, the collisional electron-ion coupling at that high density brought the ion temperature up as well. In particular in combination with pellet injection transiently ion temperatures Ti above 3 keV and close to the neoclassical limit of the W7-X magnetic configurations could be achieved. Thus enabling to test the W7-X neoclassical optimization [2]. Also the beneficial effect on impurity control by electron heating could be demonstrated.
The 140 GHz EC-wave with ordinary (O2) polarization give access to densities beyond the cut-off limit of the commonly used extra-ordinary (X2) polarized waves, but for the expense of incomplete single pass absorption for the W7-X plasma parameter. This disadvantage could be compensated by a special the multi-pass scenario, where the partially (60-70%) absorbed ECRH-beams have been reflected by specially shaped tiles and passed three times through the plasma core with an overall absorption of up to 90%. A detailed analyses of the absorption and losses for all 10 ECRH beams in the experiments enabled further optimization of the reflector tiles, thus in the next campaign an overall absorption of 95% is envisaged. This on the first glance small improvement will reduce the none-absorbed ECRH stray radiation by 50%, which is a remarkable step forward for prospective future steady state operation, since the microwave stray radiation gives an additional load to all W7-X components even if they are outside a line of sight to the plasma [3]. The O2-opereration scenario has been also routinely used for plasma operation below the X2 cutoff at densities above 0.8 1020 m-3 prohibiting the otherwise high risk of uncontrolled beam deflection in the X2-mode ECRH case. In order to keep the absorption high, the density feed-back controls for a central Te above 2 keV. In this scenario stable and stationary detachment for 24 s could demonstrated, which was only limited by the energy limit given by the uncooled plasma facing W7-X components in OP1.2. A further benefit of the O2-ECRH scenario was the compatibility with high neutral pressure at the plasma edge. Even though after the boronization of the W7-X wall no glow discharge cleaning has been performed any more the density control was never lost and the high density operation was very robust. But on the other side in the presence of the high neutral fluxes, plasma radiation and charge exchange losses pushed down the edge temperatures as shown in Fig 1.

Electron density (pink),  temperature (red) and ion temperature (blue) profile for a pure O2-ECRH plasma with gas fueling in #20180904.015.

The possible large density range enable a combined operation with pellet injection without the risk of approaching the cut-off condition for the here pellet-induced peaked density profiles. After the pellet injection phase, the transport properties are being improved for the ion and thus high plasma performance with high tripple product values have been achieved [4]. Here the ion power flux approaches the neoclassical value enabling to test the neoclassical transport optimization of W7-X.

O2 ECRH scenario in combination with pellet injection (#20170904.015). For the plasma start-up three ECRH beams are polarized in X2-mode. During the density ramp their polarization is changed into O2-mode. The gray shaded area is the overdense phase.

The neoclassical impurity transport in stellarators predicts an inward pinch and thus a impurity accumulation. Electron temperature gradient driven turbulence is counteracting here and thus in ECRH-plasmas with gas fueling no accumulation has been found [5]. In particular the laser blow off experiments estimated impurity confinement time of the order of 70-80 ms which is far below the neoclassical confinement times of 2-10s [6]. Even more in cases, where impurity accumulation has been found, like in the exclusively NBI-heated high density plasmas, additional O2-ECRH significantly flattened the otherwise peaked Impurity profiles and pushed the impurities toward the plasma edge.
The high density operation with the multi-pass O2-ECRH scenario showed an excellent plasma performance. However the maximal achieved temperature were limited by the amount of available heating power (6MW for 20s) and the respective transport parameters of the plasma scenarios. In particular the gas fed ECRH-plasmas suffered from low plasma edge temperatures, which prohibit the efficient use of magnetic confinement region. For the next operation campaign an upgrade of the available ECRH power to 10 MW and more effective multi-pass reflector tiles are planned. In particular a new more powerful (1.5 MW) gyrotron is being developed now [7] and number of gyrotrons and beamlines will be increased from 10 to 12. In addition the maximal power capability of the in-air quasi-optical transmission line is being enhanced with a strong air drying system. Plasma performance enhancement is also expected by an improved edge neutral density control with cryo pumps in the divertor pumping gap and gas valves in the divertor region. In addition a steady state pellet injector will enable continuous core fueling at low neutral edge density.
[1] M. Jakubowski et al, submitted to Phys. Rev. Lett. (2020)
[2] C. Beidler et al. in preparation (2020)
[3] H.P. Laqua et al. In Proceedings of the 28th EPS Conf. Control. Fusion and Plasma Phys.,Funchal 2001, ECA 25A, European Physical Society, Geneva 2001, 1277-1280.
[4] T.Sunn Pederson et al. Plasma Physics and Controlled Fusion, Volume 61, Number 1
[5] A. Langenberg, F. Warmer, G. Fuchert et al. PPCF 61 014030 (2019)
[6] T. Wegner et al. RSI 89, 073505 (2018);
[7] G.Gantenbein et al., this conference (2020)
This work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training program 2014-2018 and 2019-2020 under grant agreement No 633053. The views and opinions expressed herein do not necessarily reflect those of the European Commission

Affiliation Max-Planck-Institut for Plasma Physics
Country or International Organization Germany

Primary author

Heinrich Laqua (Max-Planck-Institute for Plasma Physics, Greifswald, Germany)


Dr Jurgen Baldzuhn (Max-planck Institut fuer Plasmaphysik) Dr Harald Braune (Max-Planck-Institut for Plasma Physics) Sergey Bozhenkov (Max-Planck-Institut für Plasmaphysik, Greifswald, Germany) Kai Jakob Brunner (Max-Planck-Institut für Plasmaphysik Teilinstitut Greifswald) Matthias Hirsch (Max-Planck-Institut für Plasmaphysik) Dr Udo Hoefel (Max-Planck Institut für Plasmaphysik) Jens Knauer (Max-Planck-Institut für Plasmaphysik Teilinstitut Greifswald) Andreas Langenberg (Max-Planck-Institut für Plasmaphysik,17491 Greifswald, Germany) Stefan Marsen (Max-Planck-Institut für Plasmaphysik Teilinstitut Greifswald) Dmitry Moseev (Max-Planck-Institut für Plasmaphysik) Novimir Pablant (Princeton Plasma Physics Laboratory) Dr Ekkehard Pasch (Max-Planck-Institute for Plasma Physics) Dr Torsten Stange (Max-Planck Institut für Plasmaphysik) Robert Wolf (Max-Planck-Institute for Plasma Physics) Wendelstein7-X Team (Max-Planck-Institute for Plasma Physics)

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