Variability of MHD instabilities in benign termination of high-current runaway electron beams in the JET and DIII-D tokamaks
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Open Access
- 30 March 2026
- journal article
- Published by IOP Publishing in Nuclear Fusion
- Vol. 66 (5) , 056004
Abstract
Benign termination, in which magnetohydrodynamic (MHD) instabilities deconfine runaway electrons (REs) following hydrogenic injections, is a promising strategy for mitigating dangerous RE loads after disruptions. Recent experiments on the Joint European Torus (JET) have explored this scenario at higher pre-disruptive plasma currents than are achievable on other devices, revealing challenges in obtaining benign terminations at I p ⩾ 2.5 MA. This work analyzes the evolution of these high-current RE beams and their terminating MHD events using fast magnetic sensor measurements and EFIT equilibrium reconstructions for approximately 40 JET and 20 DIII-D tokamak discharges. On JET, unsuccessful non-benign terminations occur at low edge safety factor ( q edge ≈ 2 ), and are preceded by intermittent, non-terminating MHD events at higher rational q edge . Trends in the internal inductance l i indicate more peaked RE current profiles in the high- I p non-benign population, which may hinder successful recombination through re-ionization of the companion plasma. In contrast, benign terminations on JET typically occur at higher q edge ⩾ 3 and exhibit less peaked RE current profiles. DIII-D displays a broader range of terminating edge safety factors, again correlated with the measured l i values. Across both tokamaks, the RE current peaking is therefore found to determine which MHD instability boundary is encountered, a result confirmed by linear resistive MHD modeling with the CASTOR3D code. Measured growth rates are similar for benign and non-benign cases, indicating that ideal MHD timescales at low density after hydrogenic injection do not alone explain efficient RE deconfinement. Instead, non-benign cases are most readily characterized by their comparably lower overall MHD perturbation amplitudes δ B . These observations suggest that the interplay between ideal and resistive dynamics governs the termination process, with implications for extrapolating benign RE termination to high- I p reactor scenarios.Keywords
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Funding Information
- Swiss State Secretariat for Education, Research and Innovation
- 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 (DE-FC02-04ER54698)
- EUROfusion Consortium, funded by the European Union via the Euratom Research and Training Programme (Grant Agreement No 101052200 EUROfusion)
This publication has 33 references indexed in Scilit:
- Spurious radiated power signal following massive material injections in JET and the effect of neutral gas pressure on resistive bolometersReview of Scientific Instruments, 2024
- Non-linear dynamics of the double tearing modePhysics of Plasmas, 2023
- Optimizing the differential connection schemes for detecting 3D magnetic perturbations in DIII-DReview of Scientific Instruments, 2021
- Loss of relativistic electrons when magnetic surfaces are brokenPhysics of Plasmas, 2016
- Runaway electrons and the evolution of the plasma current in tokamak disruptionsPhysics of Plasmas, 2006
- Theory for avalanche of runaway electrons in tokamaksNuclear Fusion, 1997
- Disruptions in JETNuclear Fusion, 1989
- Three-dimensional free boundary calculations using a spectral Green's function methodComputer Physics Communications, 1986
- Separation of β̄pand ℓiin tokamaks of non-circular cross-sectionNuclear Fusion, 1985
- Runaway electrons in toroidal dischargesNuclear Fusion, 1979