Measurements of X-point radiator and MARFEs using the high-field side Thomson Scattering diagnostic at ASDEX Upgrade
POSTER
Abstract
To ensure the longevity of the plasma-facing components and the divertor in a fusion reactor, it is crucial to maintain the incident heat flux to those surfaces at tolerable levels. Therefore, a fully detached plasma state is preferable. In this state, an X-point radiator (XPR) can be observed at ASDEX Upgrade (AUG): a highly radiating, poloidally localized region within the separatrix near the geometrical X-point [U. Stroth et al. NF 62 2022]. Controlling this XPR provides access to a detached scenario that has many of the properties required for a reactor scenario in ITER or DEMO. However, if the XPR migrates too far into the confined plasma region, it can become unstable and mutate into a MARFE, which moves from the X-point region to the high-field side of the plasma, and ususally terminates in a plasma disruption. A deeper understanding of the XPR/MARFE physics is therefore critical for predictive control in future fusion devices. This requires local measurements of electron temperature Te and density ne on the high-field side, which we have performed at AUG for the first time in over 30 years using the Thomson scattering diagnostic [B. Kurzan et al. RSI 82 2011]. Te and ne are measured at 15 vertical positions, predominantly below the midplane (ρpol > 0.9). During MARFE phases in the confined region, electron temperatures below 10 eV and densities exceeding 1020 m-3 are observed. Additionally, we present a comparison with the Thomson scattering channels located in the divertor [B. Kurzan et al. JINST 16 2021] in order to analyze the behavior of the XPR/MARFE.
Presenters
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Joey Kalis
Max Planck Institute for Plasma Physics
Authors
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Joey Kalis
Max Planck Institute for Plasma Physics
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Bernd Kurzan
Max Planck Institute for Plasma Physics
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Matthias Willensdorfer
Max Planck Institute for Plasma Physics
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Bernhard Sieglin
Max Planck Institute for Plasma Physics, Garching, Germany
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Marc Maraschek
Max Planck Institute for Plasma Physics, Garching, Germany
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Elisabeth Wolfrum
Max-Planck-Institut für Plasmaphysik, Boltzmannstr. 2, 85748 Garching, Germany
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Rachael M. McDermott
Max Planck Institute for Plasma Physics
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Ou Pan
Max Planck Institute for Plasma Physics, Garching, Germany