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DOE OSTI · 2997570

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

Scotti, Filippo [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000201969919)·Marinoni, Alessandro [University of California, San Diego, CA (United States)] (ORCID:0000000310045782)·McLean, Adam G. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000206974397)·Nelson, A. O. [Columbia University, New York, NY (United States)] (ORCID:0000000296121936)·Paz-Soldan, Carlos [Columbia University, New York, NY (United States)] (ORCID:0000000150694934)·Thome, K. E. [General Atomics, San Diego, CA (United States)] (ORCID:0000000248013922)·Zhao, M. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000194877644)·Allen, S. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)]·Austin, Max [University of Texas, Austin, TX (United States)] (ORCID:0000000200178605)·Burke, M. G. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000176193724)·Bykov, I. [General Atomics, San Diego, CA (United States)] (ORCID:0000000165196081)·Chrystal, Colin [General Atomics, San Diego, CA (United States)] (ORCID:0000000330498658)·Eldon, David [General Atomics, San Diego, CA (United States)] (ORCID:0000000318950648)·Fenstermacher, M. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000156357330)·Hyatt, A. [General Atomics, San Diego, CA (United States)]·Glass, Fenton [General Atomics, San Diego, CA (United States)] (ORCID:0000000311011859)·Lasnier, C. J. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000271092278)·Lore, Jeremy [Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)] (ORCID:000000029192465X)·Leonard, A. [General Atomics, San Diego, CA (United States)] (ORCID:0000000193561074)·Murphy, Christopher [General Atomics, San Diego, CA (United States)]·Osborne, Thomas [General Atomics, San Diego, CA (United States)] (ORCID:0000000326414597)·Sauter, O. [École Polytechnique Fédérale de Lausanne (EPFL) (Switzerland)] (ORCID:0000000200996675)·Truong, D. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000285732539)·Wang, Huiqian Q. [General Atomics, San Diego, CA (United States)] (ORCID:0000000319202799)·Wilcox, Robert [Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)] (ORCID:0000000313691739)

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.

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BibTeXRIS

Scotti, Filippo [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000201969919), Marinoni, Alessandro [University of California, San Diego, CA (United States)] (ORCID:0000000310045782), McLean, Adam G. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000206974397), Nelson, A. O. [Columbia University, New York, NY (United States)] (ORCID:0000000296121936), Paz-Soldan, Carlos [Columbia University, New York, NY (United States)] (ORCID:0000000150694934), Thome, K. E. [General Atomics, San Diego, CA (United States)] (ORCID:0000000248013922), Zhao, M. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000194877644), Allen, S. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)], Austin, Max [University of Texas, Austin, TX (United States)] (ORCID:0000000200178605), Burke, M. G. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000176193724), Bykov, I. [General Atomics, San Diego, CA (United States)] (ORCID:0000000165196081), Chrystal, Colin [General Atomics, San Diego, CA (United States)] (ORCID:0000000330498658), Eldon, David [General Atomics, San Diego, CA (United States)] (ORCID:0000000318950648), Fenstermacher, M. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000156357330), Hyatt, A. [General Atomics, San Diego, CA (United States)], Glass, Fenton [General Atomics, San Diego, CA (United States)] (ORCID:0000000311011859), Lasnier, C. J. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000271092278), Lore, Jeremy [Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)] (ORCID:000000029192465X), Leonard, A. [General Atomics, San Diego, CA (United States)] (ORCID:0000000193561074), Murphy, Christopher [General Atomics, San Diego, CA (United States)], Osborne, Thomas [General Atomics, San Diego, CA (United States)] (ORCID:0000000326414597), Sauter, O. [École Polytechnique Fédérale de Lausanne (EPFL) (Switzerland)] (ORCID:0000000200996675), Truong, D. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000285732539), Wang, Huiqian Q. [General Atomics, San Diego, CA (United States)] (ORCID:0000000319202799), Wilcox, Robert [Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)] (ORCID:0000000313691739). 2025-09-19. Divertor characterization and access to dissipative divertor conditions in negative triangularity discharges in DIII-D. https://doi.org/10.1088/1361-6587%2Fadf881

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Effect of outer divertor leg detachment on the high field side scrape-off layer in DIII-D and ASDEX Upgrade

In this work, evidence is presented that detachment of the outer divertor leg leads to a reduction of electron density and neutral pressure in the high-field side (HFS) scrape-off layer (SOL) of the ASDEX Upgrade (AUG) and DIII-D tokamaks with ion $B$ x $∇B$ drift directed toward the X-point (favorable configuration). These results are observed across multiple diagnostics and without the use of impurity seeding to reach detachment. In AUG, outer divertor leg detachment correlates with a decrease in electron density near the separatrix at the inner midplane, measured with HFS reflectometry. A concurrent reduction in inner divertor density and neutral pressure at the inner target is observed using divertor Thomson scattering and neutral pressure gauges. These effects are present in both L- and H-mode plasmas. In DIII-D, a similar reduction is detected through analysis of line-integrated hydrogenic emission measured by multiple diagnostics in the HFS SOL close to the separatrix. The consistent trends in both devices indicate that high electron density and strong hydrogenic emissivity in the HFS SOL are common features of H-mode plasmas in the favorable configuration, independent of wall material and divertor geometry. In L-mode plasmas, the reduction in electron density and neutral pressure is not observed in DIII-D, possibly due to differences in wall material. These results emphasize the importance of the divertor state in determining the two-dimensional neutral distribution and edge fueling.

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