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Overview of the DIII-D Negative Triangularity Campaign

ORAL

Abstract

In early 2023, a dedicated multi-week experimental campaign was conducted to qualify the negative triangularity (NT) scenario for future reactors on the DIII-D tokamak after the installation of graphite-tile armor on the low-field-side lower outer wall. During this campaign, high confinement (H98y,2≥1), high current (q95<3), and high normalized pressure plasmas (βN>2.5) were achieved at high-injected-power in strongly NT-shaped plasmas with δavg= - 0.5 and a lower outer divertor X-point that also demonstrated high normalized density (ne/nGW≤2), particle confinement comparable to energy confinement, and a detached divertor without impurity seeding, all while maintaining a non-ELMing NT-edge with an electron temperature pedestal, exceeding that of typical low-confinement (L-mode) plasmas. This reactor-relevant regime is accessed over a wide range of DIII-D operational space (plasma current, toroidal field, electron density and pressure) in contrast to other high-performance non-ELMing scenarios that have narrower operating windows. Two scenarios were developed: an inductive high-gain plasma with usually lower q95 and sawteeth and an advanced quasi-steady-state plasma with higher q95=4 that were sawtooth-free, indicating qmin>1 was obtained.

Presenters

  • Kathreen E Thome

    General Atomics

Authors

  • Kathreen E Thome

    General Atomics

  • Max E Austin

    University of Texas at Austin, University of Texas – Austin

  • Alan W Hyatt

    General Atomics - San Diego

  • Alessandro Marinoni

    Massachusetts Institute of Technology MIT

  • Andrew O Nelson

    Columbia University

  • Carlos A Paz-Soldan

    Columbia University

  • Filippo Scotti

    Lawrence Livermore Natl Lab

  • J. L Barr

    General Atomics - San Diego, General Atomics

  • William Boyes

    Columbia University

  • Livia Casali

    University of Tennessee Knoxville

  • Colin Chrystal

    General Atomics - San Diego

  • Tyler B Cote

    General Atomics

  • Siye Ding

    General Atomics

  • Xiaodi Du

    General Atomics - San Diego

  • David Eldon

    General Atomics - San Diego, General Atomics

  • Darin R Ernst

    Massachusetts Institute of Technology MIT, Massachusetts Institute of Technology MI

  • Andrea M. M Garofalo

    General Atomics, General Atomics - San Diego

  • Rongjie Hong

    UCLA

  • Filipp Khabanov

    Wisconsin-Madison, University of Wisconsin-Madison, University of Wisconsin–Madison, University of Wisconsin- Madison, UWM

  • Gerrit J Kramer

    Princeton Plasma Physics Laboratory

  • Charlie Lasnier

    Lawrence Livermore National Laboratory, LLNL, Lawrence Livermore National Lab

  • Priyansh Lunia

    Columbia University

  • George R McKee

    University of Wisconsin - Madison, UWisc. Madison

  • Adam McLean

    Lawrence Livermore National Laboratory, Lawrence Livermore Natl Lab

  • Saskia Mordijck

    College of William and Mary

  • Michio Okabayashi

    Princeton Plasma Physics Laboratory

  • Olivier Sauter

    EPFL, Ecole Polytechnique Federale de Lausanne, Swiss Plasma Center, EPFL-SPC

  • Lothar Schmitz

    University of California, Los Angeles

  • Daisuke Shiraki

    Oak Ridge National Lab, Oak Ridge National Laboratory, General Atomics - San Diego

  • Samuel Stewart

    University of Wisconsin - Madison, University of Wisconsin-Madison

  • Yuki Takemura

    NIFS

  • Dinh Truong

    Lawrence Livermore National Laboratory, Sandia National Laboratories

  • Tom H Osborne

    General Atomics, General Atomics - San Diego

  • Huiqian Wang

    General Atomics, General Atomics - San Diego

  • Theresa M Wilks

    MIT-PSFC, MIT

  • Menglong Zhao

    Lawrence Livermore National Laboratory