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3–6 Sept 2019
Shizuoka City, Japan
Europe/Vienna timezone
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Excitation of elliptical and toroidal AE modes by 3 He - ions of the MeV energy range in hydrogen - rich JET plasma

6 Sept 2019, 11:10
25m
Shizuoka City, Japan

Shizuoka City, Japan

Board: O-19
Oral (Plenary Session) Control of Energetic Particle Confinement Plenary

Speaker

Dr Vasily Kiptily (United Kingdom Atomic Energy Authority)

Description

Authors: V.G.Kiptily, Ye.Kazakov, M.Nocente, M.Fitzgerald, S.E.Sharapov, A.E.Shevelev, and JET Contributors

Excitation of Elliptical AEs (EAEs) and TAEs has been observed in hydrogen-rich (nH/nH+nD ~70-90%) JET discharges of so-called “three-ion scenario”, i.e.D-(3He)-H three ion ICRH scenario [1]. This scenario is characterized by a strong absorption of radio frequency waves at very low concentrations of the resonant 3He-ions. In the experiments, core localized TAEs with frequency f_TAE≈ 280 kHz were observed. Following the phase with the TAE excitation, EAEs at higher frequencies, f_EAE≈ 550-580 kHz, and with mode numbers n=±1, ±3, ±5 were seen. These high frequency modes indicate that a MeV range population of trapped energetic ions was present in the plasma interacting with the modes via the trapped particle resonances. The experimental evidence of the existence of the MeV-energy 3He-ions able to excite the AEs is provided by neutron and gamma-ray diagnostics as well as fast ion loss (FILD) measurements. It was found that the anomalous DD neutron rate in the ICRF-only heated plasma is provided by population of energetic deuterons formed via elastic head-on scattering of the MeV 3He-ions on deuterium (the knock-on effect): D(3He,3He)D knock-on=> D(D_knock-on,n)3He. Gamma-ray diagnostics [2] show that some neutrons are also generated in the nuclear reaction 9Be(3He,n)11C, which takes place with 3He-ions in the MeV-range. The fast ion loss detector [3] indicates that the MeV-range 3He-ion losses related to the core localized TAEs ended with a spike associated with a monster sawtooth, after which the losses correlated to the EAE modes were observed. Analysis of FILD data indicates that the lost 3He-ion energies exceed 2 MeV. The back-in-time orbit analysis of the FILD data shows that the TAE-induced losses of 3He-ions are localised in the plasma centre (R≈3.0 m). However, the losses of 3He-ions associated with the EAEs are coming from R≈3.2-3.4 m. Results of MHD analysis are consistent with the experimental data showing that the MeV 3He ions are resonant when interacting with TAEs and EAEs.
References
[1] Ye.O. Kazakov, D. Van Eester, R. Dumont and J. Ongena, Nucl. Fusion 55 (2015) 032001;
[2] V.G. Kiptily, F.E. Cecil and S.S. Medley, Plasma Phys. Control. Fusion 48 (2006) R59;
[3] D. Darrow et al. Rev. Sci. Instrum. 77 (2006) 10E701.

Country or International Organization United Kingdom

Primary authors

Dr Vasily Kiptily (United Kingdom Atomic Energy Authority) Yevgen Kazakov (Laboratory for Plasma Physics, LPP-ERM/KMS) Massimo Nocente (Dipartimento di Fisica, Università di Milano-Bicocca) Dr Michael Fitzgerald (CCFE) Sergei Sharapov (Culham Centre for Fusion Energy) Alexander Shevelev (Ioffe Institute)

Presentation materials