DOI: 10.7910/dvn/tfste6
title: Turbulence suppression at extreme plasma densities on DIII-D and EAST

description: Recent high-poloidal-beta (high-beta-P) experiments on DIII-D and EAST have made coordinated breakthroughs for high confinement quality at high density near the Greenwald limit. Density gradient amplification of turbulence suppression at high beta-P can explain both of these achievements. Experiments on DIII-D have achieved Greenwald fraction (fGr=line-averaged density/Greenwald density) above 1 simultaneously with normalized energy confinement (H98y2) around 1.5, as required in fusion reactor designs but never before verified in tokamak experiments with divertor configuration. A synergy between increased H98y2 and fGr is observed with strong gas puffing, due to the build-up of an internal transport barrier at large radius in the temperature and density channels. Transport simulations reveal that the favorable trend of reduced turbulent energy transport at higher density is only expected when increasing the density gradient at high local safety factor and high beta, thus at high beta-P to ensure strong alpha-stabilization. These conditions are crucial to many conceptual designs for steady-state reactors. New experiments on EAST have nearly doubled the ion temperature at fGr~0.9, consistent with predict-first modeling results based on the same physics revealed from the DIII-D analysis. All previous EAST long-pulse H-modes have Ti&lt;&lt;Te near plasma axis. Transport modeling indicates that the profiles are limited by ion-temperature-gradient (ITG) modes at mid-radius. The modeling also suggested potential solutions, including reducing magnetic shear, enhancing density gradients and higher impurity concentration. Following this guidance, EAST experiments directly show a strong enhancement of Ti achieved with a combination of a 2nd plasma current ramp-up, a density gradient increase, and a Zeff perturbation by a short pulse (100 ms) of impurity injection, as predicted by the earlier modeling.
description: CITATION: Phys. Plasmas 32, 022502 (2025)<br><br>DOI: https://doi.org/10.1063/5.0235599<br><br>PSFC REPORT PSFC/JA-25-18<br><br>This material is based upon work 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-SC0010685, DE-FC02-04ER54698, DE-AC52-07NA27344, DE-FG02-04ER54761, DE-AC02-09CH11466 and DE-SC0016154. This report was 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 is also supported by DoE award: DE-SC0010492.<br><br>If this record does not contain the full text, then the manuscript has been embargoed by the publisher thus restricting open access for 12 to 24 months after publication.