[1] Fasoli A, Gormenzano C, Berk H L, et al. ITER Physics,
Chapter 5: Physics of energetic ions [J]. Nuclear Fusion,
2007, 47(6): S267‒S268.
[2] Pinches S D, Chapman I T, Lauber P W, et al. Energetic
ions in ITER plasmas [J]. Phys. Plasmas, 2015, 22(2):
021807.
[3] Gorelenkov N N, Pinches S D, Toi K, et al. Energetic
particle physics in fusion research in preparation for
burning plasma experiments [J]. Nucl. Fusion, 2014,
54(12): 125001.
[4] Igochine V. Active control of magneto-hydrodynamic
instabilities in hot plasmas [M]. Springer Heidelberg
New York Dordrecht London, 2015. 260.
[5] White R B. The Theory of toroidally confined plasmas
(3rd edn) [M]. Singapore: World Scientific, 2014. 80.
[6] Yu Q, Günter S, Scott B D. Numerical modeling of linear
drift-tearing mode stability [J]. Phys. Plasmas., 2003,
10(3): 797‒810.
[7] Wang X J, Yu Q, Zhang X, et al. Numerical modelling on
stabilizing large magnetic island by RF current for
disruption avoidance [J]. Nucl. Fusion, 2018, 58(1):
016045.
[8] White R B. Modification of particle distributions by
MHD instabilities I [J]. Commun Nonlinear Sci Numer
Simulat, 2012, 17: 2200.
[9] White R B. Modification of particle distributions by
magnetohydrodynamic instabilities II [J]. Plasma Phys.
Contr. Fusion, 2011, 53(8): 085018.
[10] White R B. Particle distribution modification by low
amplitude modes [J]. Plasma Phys. Contr. Fusion, 2010,
52(4): 045012.
[11] White R B, Duarte V N, Gorelenkov N N, et al.
Simulation of Alfvénic avalanche onset in NSTX [J].
Phys. Plasmas, 2020, 27(2): 022117.
|