Bifurcation-like transition of divertor conditions induced by X-point radiation in KSTAR L-mode plasmas

Jae Sun Park, Richard Pitts, Juhyeok Jang, Yoon Seong Han, Wonho Choe, Jeremy Lore, Junghoo Hwang, Jun Gyo Bak, June Woo Juhn, Suk Ho Hong

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10 Scopus citations

Abstract

Density ramps with ion grad B drift directed into lower single null KSTAR L-mode plasmas are associated with a simultaneous and abrupt reduction of the divertor particle flux on both low- and high-field-side targets when the mid-plane line averaged electron density reaches a given level. Target embedded Langmuir probe signals show a clear ‘cliff edge’ behavior similar to that observed in the divertor target electron temperature in DIII-D H-mode plasmas (Eldon et al 2017 Nucl. Fusion 57 066039; McLean et al 2015 J. Nucl. Mater. 463 533-6). The collapse of the particle flux is observed along the whole divertor target area (from private flux region to the far scrape-off layer (SOL)). The critical upstream density of this target flux cliff is invariant under fuel gas throughput modulation. The transition along the cliff occurs in tens of milliseconds. With the cliff, carbon impurities and deuterium neutrals transported through the X-point to the core produce a strong radiation spot near the X-point, seen on bolometric signals, and increase the upstream density. The experimental observations are consistent with time-dependent SOLPS-ITER simulations, which also demonstrate an abrupt transition of the target flux and upstream density with the increase in X-point radiation. The timescale of the cliff predicted by SOLPS-ITER is consistent with the experiment, although, it is influenced by gas throughput or time-dependent numerical methods. In the L-mode phase space of separatrix electron density and temperature, branches are divided based on target temperature, because the latter is strongly coupled to the radiation front and ionization front due to the monotonic characteristic of the parallel electron temperature distribution. Since the H-mode condition operates at a much higher upstream density and electron temperature in phase space, dissipation from sputtered carbon alone leads to the density limit before reaching the X-point radiation condition. This is therefore consistent with the fact that cliffs have never been observed in H-mode KSTAR experiments.

Original languageEnglish
Article number086018
JournalNuclear Fusion
Volume63
Issue number8
DOIs
StatePublished - Aug 2023

Funding

This work was supported by the National R&D Program through the National Research Foundation of Korea (NRF), funded by the Ministry of Science, ICT (NRF-2014M1A7A1A03045092). The simulation part of research sponsored by the Laboratory Directed Research and Development program of Oak Ridge National Laboratory, managed by UT-Battelle LLC for the US Department of Energy under Contract DE-AC05-00OR22725. The views and opinions expressed herein do not necessarily reflect those of the ITER Organization. This research was supported by the R&D Program of ‘KSTAR Experimental Collaboration and Fusion Plasmas Research (EN2301-14)’ through the Korea Institute of Fusion Energy (KFE) funded by the Korea Ministry of Science and ICT (MSIT). This manuscript has been authored in part by UT-Battelle, LLC, under contract DE-AC05-00OR22725 with the US Department of Energy (DOE). The publisher acknowledges the US government license to provide public access under the DOE Public Access Plan ( http://energy.gov/downloads/doe-public-access-plan ).

Keywords

  • KSTAR
  • SOLPS-ITER
  • X-point radiation
  • cliff edge
  • time-dependent SOLPS

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