Abstract

This paper summarizes the physical principles behind the novel three-ion scenarios using radio frequency waves in the ion cyclotron range of frequencies (ICRF). We discuss how to transform mode conversion electron heating into a new flexible ICRF technique for ion cyclotron heating and fast-ion generation in multi-ion species plasmas. The theoretical section provides practical recipes for selecting the plasma composition to realize three-ion ICRF scenarios, including two equivalent possibilities for the choice of resonant absorbers that have been identified. The theoretical findings have been convincingly confirmed by the proof-of-principle experiments in mixed H–D plasmas on the Alcator C-Mod and JET tokamaks, using thermal 3He and fast D ions from neutral beam injection as resonant absorbers. Since 2018, significant progress has been made on the ASDEX Upgrade and JET tokamaks in H–4He and H–D plasmas, guided by the ITER needs. Furthermore, the scenario was also successfully applied in JET D–3He plasmas as a technique to generate fusion-born alpha particles and study effects of fast ions on plasma confinement under ITER-relevant plasma heating conditions. Tuned for the central deposition of ICRF power in a small region in the plasma core of large devices such as JET, three-ion ICRF scenarios are efficient in generating large populations of passing fast ions and modifying the q-profile. Recent experimental and modeling developments have expanded the use of three-ion scenarios from dedicated ICRF studies to a flexible tool with a broad range of different applications in fusion research.

Highlights

  • Strong magnetic fields are used to confine plasmas in fusion devices

  • This paper summarizes the physical principles behind the novel three-ion scenarios using radio frequency waves in the ion cyclotron range of frequencies (ICRF)

  • For this series of ASDEX Upgrade (AUG) experiments with off-axis three-ion ICRF heating, L–H transitions were generally reached at PLH % 2–3 MW, which is similar to earlier observations with hydrogen neutral beam injection (NBI) and electron cyclotron range of frequencies (ECRF) heating in H-4He plasmas on AUG.[55]

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Summary

INTRODUCTION

Strong magnetic fields are used to confine plasmas in fusion devices. As a result of the Lorentz force, plasma ions and electrons gyrate around the magnetic field lines with a local characteristic cyclotron frequency xcs 1⁄4 qsB/ms, where qs and ms are the charge and the mass of the particle and B is the local value of the magnetic field. The distance to the IIH layer gets too large for both plasma ion species and they can no longer resonate at the region with an enhanced jEþj Under these conditions, ICRF heating via mode conversion becomes dominant, where launched RF fast waves undergo a. At sufficiently large concentrations of the minority ion species, the distance between the IIH layer and the minority cyclotron resonance becomes too large such that minority ions can no longer resonate in the vicinity of the region with enhanced jEþj and electron heating via mode conversion is usually realized.[12,15] By extending the plasma composition, three-ion ICRF scenarios offer a method to transform local electron heating via mode conversion into an effective technique for ion cyclotron heating in multi-ion species plasmas with a range of applications, as discussed in this paper. Tornado TAEs, and ellipticity-induced AE (EAEs) were excited by multi-MeV 3He ions generated with the three-ion ICRF scenario

Proof-of-principle experiments with resonant fast
RECENT PROGRESS WITH APPLICATIONS OF THREE-ION ICRF SCENARIOS
Efficient generation of passing fast ions and fast-ion current drive
Toward ITER needs
Optimization of fast-ion studies with three-ion ICRF scenarios on AUG
PROMISING APPLICATIONS FOR FUSION RESEARCH
A tool for the fast-ion driven MHD modes and turbulence studies
A tool to modify the q-profile in the plasma core
Bulk ion heating in D–T plasmas
Revisiting the parasitic absorption by alphas in D–T plasmas
Extending H-mode access in hydrogen majority plasmas in ITER
Findings
SUMMARY AND CONCLUSIONS
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