[1] [1] SAUTER
O, WESTERHOF E, MAYORAL M L, et al. Control of neoclassical tearing modes by
sawtooth control [J]. Physical Review Letters, 2002, 88(10): 105001.
[2] [2] BUTTERY
R J, HENDER T C, HOWELL D F, et al. Onset of neoclassical tearing modes on JET [J].
Nuclear Fusion, 2003, 43(2): 69.
[3] [3] NAVE M
F F, KOSLOWSKI H R, CODA S, et al. Exploring a small sawtooth regime in Joint
European Torus plasmas with counterinjected neutral beams [J]. Physics of
Plasmas, 2006, 13(1): 014503.
[4] [4] CHAPMAN
I, HENDER T, SAARELMA S, et al. The effect of toroidal plasma rotation on
sawteeth in MAST [J]. Nuclear Fusion, 2006, 46(12): 1009.
[5] [5] CHAPMAN
I T, PINCHES S D, KOSLOWSKI H R, et al. Sawtooth stability in neutral beam
heated plasmas in TEXTOR [J]. Nuclear Fusion, 2008, 48(3): 699-785.
[6] [6] IKEDA
Y, IDE S, SUZUKI T, et al. ECRF experiments for local heating and current drive
by fundamental O-mode launch from the low-field side on JT-60U [J]. Nuclear
Fusion, 2002, 42(4): 375-382.
[7] [7] ANGIONI
C, GOODMAN T P, HENDERSON M A, et al. Effects of localized electron heating and
current drive on the sawtooth period [J]. Nuclear Fusion, 2003, 43(6): 455-468.
[8] [8] MUCK
I, GOODMAN T P, MARASCHEK M, et al. Sawtooth control experiments on ASDEX
Upgrade [J]. Plasma Physics and Controlled Fusion, 2005, 47(10): 1633.
[9] [9] PIRON
C, MARTIN P, BONFIGLIO D, et al. Interaction of external n=1 magnetic
fields with the sawtooth instability in low-q RFX-mod and DIII-D
tokamaks [J]. Nuclear Fusion, 2016, 56(10): 106012.
[10] [10] BONDESON
A, BUSSAC M N. Stability of the N=1 ideal internal kink for large aspect
ratio shafranov equilibria [J]. Nuclear Fusion, 1992, 32(3): 513.
[11] [11] PORCELLI
F. Fast particle stabilisation [J]. Plasma Physics & Controlled Fusion,
1991, 33(13): 1601.
[12] [12] WHITE
R B, RUTHERFORD P H, COLESTOCK P, et al. Sawtooth stabilization by energetic
trapped particles [J]. Physical Review Letters, 1988, 60(20): 2038.
[13] [13] WHITE
R B, BUSSAC M N, ROMANELLI F. High-beta, sawtooth-free tokamak operation using
energetic trapped particles [J]. Physical Review Letters, 1989, 62(5): 539.
[14] [14] KERNER
W, GRUBER R, TROYON F. Numerical study of the internal kink mode in tokamaks [J].
Physical Review Letters, 1980, 44(8): 536-540.
[15] [15] HASTIE
R J, HENDER T C, CARRERAS B A, et al. Stability of ideal and resistive internal
kink modes in toroidal geometry [J]. Physics of Fluids, 1987, 30(6): 1756-1766.
[16] [16] HOWL
W, TURNBULL A D, TAYLOR T S, et al. Sensitivity of the kink instability to the
pressure profile [J]. Physics of Fluids B: Plasma Physics, 1992, 4(7):
1724-1734.
[17] [17] TURNBULL
A D, TAYLOR T S, CHU M S, et al. Synergism between cross-section and profile
shaping in beta optimization of tokamak equilibria with negative central shear [J].
Nuclear Fusion, 1998, 38(10): 1467-1486.
[18] [18] CHAPMAN
I T, GRAVES J P, WAHLBERG C. The effect of plasma profile variation on the
stability of the n=1 internal kink mode in rotating tokamak plasmas [J].
Nuclear Fusion, 2010, 50(2): 025018.
[19] [19] REN Z,
LIU J, WANG F, et al. Influence of toroidal rotation on the tearing mode in
tokamak plasmas [J]. Plasma Science and Technology, 2020, 22(6): 85-91.
[20] [20] 毕海亮. 等离子体旋转对q=1磁流体不稳定性的影响[D]. 大连: 大连理工大学, 2017.
[21] [21] ZHANG
W, MA Z, ZHANG H, et al. Role of Hall effect on the resistive kink mode in
tokamaks [J]. Plasma Physics and Controlled Fusion, 2020, 62(2): 025030.
[22] [22] ZHANG
W, MA Z W, ZHANG H W, et al. Dynamic evolution of resistive kink mode with
electron diamagnetic drift in tokamaks [J]. Physics of Plasmas, 2019, 26(4): 042514.
[23] DUAN L, WANG X, ZHONG X. A high-order cut-cell method for
numerical simulation of hypersonic boundary-layer instability with surface
roughness [J]. Journal of Computational Physics, 2010, 229(19): 7207-7237.
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