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Comparing local plasma density and temperature evolution during sawtooth crash events in DIII-D

POSTER

Abstract

The sawtooth crash in fusion plasmas leads to a fast drop in core electron temperature, and several models have been proposed for the fast temperature relaxation, including fast magnetic reconnection provided by two-fluid effects or the plasmoid instability, or growth of higher-mode-number pressure driven instabilities. Experiments were conducted at DIII-D through the Frontier Science program where the Beam Emission Spectroscopy (BES) system was used for 2-D localized density measurements near the inversion layer (q=1 surface) during sawtooth. We analyzed the BES data by doing channel cross-calibration and subtraction of edge light [Bose et. al. to be submitted to Rev. Sci. Instrum. (2021)] to obtain time-domain movies of the plasma density evolution. The observations show that a (1,1) structure with high plasma density grows just before the temperature crashes and persists for a few plasma rotations afterward. We correlated the evolution of localized plasma density (BES), temperature (ECEI), and magnetic field (from external magnetics) in time to understand the physics of sawtooth crash. Initial MHD simulation results to complement the experimental finding are presented.

Publication: Two-dimensional density evolution local to the inversion layer during sawtooth crash using Beam Emission Spectroscopy at DIII-D tokamak, S. Bose, W. Fox, D. Liu, Z. Yan, G. McKee, A. Goodman, and H. Ji, to be submitted (2021).

Presenters

  • Dingyun Liu

    Princeton University

Authors

  • Dingyun Liu

    Princeton University

  • William R Fox

    Princeton Plasma Physics Laboratory, Princeton Plasma Physics Laboratory (PPPL), USA, Princeton University

  • Sayak Bose

    Princeton Plasma Physics Laboratory, Princeton University

  • Zheng Yan

    University of Wisconsin - Madison, University of Wisconsin, Madison

  • George R McKee

    University of Wisconsin - Madison, University of Wisconsin, Madison

  • Aaron Goodman

    Princeton University, Princeton university

  • Hantao Ji

    Princeton University

  • Valentin Igochine

    Max Planck Institute for Plasma Physics

  • Yilun Zhu

    University of California, Davis

  • Stephen C Jardin

    Princeton Plasma Physics Laboratory

  • Nathaniel M Ferraro

    Princeton Plasma Physics Laboratory