Divertor characterization and access to dissipative divertor conditions in negative triangularity discharges in DIII-D

  • F. Scotti
  • , A. Marinoni
  • , A. G. McLean
  • , A. O. Nelson
  • , C. Paz-Soldan
  • , K. E. Thome
  • , M. Zhao
  • , S. Allen
  • , M. Austin
  • , M. G. Burke
  • , I. Bykov
  • , C. Chrystal
  • , D. Eldon
  • , M. Fenstermacher
  • , A. Hyatt
  • , F. Glass
  • , C. J. Lasnier
  • , J. Lore
  • , A. Leonard
  • , C. Murphy
  • T. Osborne, O. Sauter, D. Truong, H. Q. Wang, R. Wilcox

Research output: Contribution to journalArticlepeer-review

1 Scopus citations

Abstract

Reduced radial transport, short midplane-to-target parallel connection lengths, and a strong effect of cross-field drifts were responsible for the high densities required for detachment in strong negative triangularity (NT) configurations in DIII-D. Dissipative divertor conditions were achieved in NT discharges at different triangularity, injected power, plasma current, and toroidal field direction. Differences between negative and positive triangularity (PT) discharges are analyzed in this paper to understand the requirements for access to detached divertor conditions: power balance, geometry, radial transport and effect of cross-field particle drifts. Parametric dependencies of access to detachment on plasma current and power flowing into the scrape-off layer remained similar in negative and PT and impurity seeding was observed to reduce the density needed to detach by up to 30% at the expense of core impurity dilution. The impact of triangularity on core-edge integration was tested varying bottom triangularity at fixed top triangularity. The high density needed to detach was not intrinsic to the NT edge as shapes with positive lower triangularity and negative upper triangularity were able to detach at lower upstream densities while maintaining an ELM-free NT edge. Confinement degradation at deeper detachment levels was however observed in all NT shapes, often associated with radiation instabilities.

Original languageEnglish
Article number095030
JournalPlasma Physics and Controlled Fusion
Volume67
Issue number9
DOIs
StatePublished - Sep 30 2025

Funding

This material was supported by the U.S. Department of Energy, Office of Science, Office of Fusion Energy Sciences, using the DIII-D National Fusion Facility, a DOE Office of Science user facility, under Awards DE-AC52-07NA27344, DE-FC02-04ER54698, DE-AC05-00OR22725, DE-SC0022270, DE-SC0016154, DE-FG02-97ER54415. This report is prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof. This work has been carried out within the framework of the EUROfusion Consortium, via the Euratom Research and Training Programme (Grant Agreement No 101052200 - EUROfusion) and funded by the Swiss State Secretariat for Education, Research and Innovation (SERI). Views and opinions expressed are however those of the author(s) only and do not necessarily reflect those of the European Union, the European Commission, or SERI. Neither the European Union nor the European Commission nor SERI can be held responsible for them.

Keywords

  • detachment
  • divertor
  • negative triangularity
  • plasma

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