|
[1] FEDERICI G, ANDREW P,
BARABASCHI P, et al. Key ITER plasma edge and plasma-material interaction
issues [J]. Journal of Nuclear Materials, 2003, 313: 11-22.
[2] GAROFALO A M, SOLOMON W M,
PARK J K, et al. Advances towards QH-mode viability for ELM-stable operation in
ITER [J]. Nuclear Fusion, 2011, 51(8): 083018.
[3] WHYTE D G, HUBBARD A E, HUGHES
J W, et al. I-mode: an H-mode energy confinement regime with L-mode particle
transport in Alcator C-Mod [J]. Nuclear Fusion, 2010, 50(10): 105005.
[4] HUBBARD A E, WHYTE D G,
CHURCHILL R M, et al. Edge energy transport barrier and turbulence in the
I-mode regime on Alcator C-Mod [J]. Physics of Plasmas, 2011, 18(5): 056115.
[5] WOLFRUM E, BERNERT M, BOOM J
E, et al. Characterization of edge profiles and fluctuations in discharges with
type-II and nitrogen-mitigated edge localized modes in ASDEX Upgrade [J].
Plasma Physics & Controlled Fusion, 2011, 53(8): 085026.
[6] XU G S, YANG Q Q, YAN N, et
al. Promising high-confinement regime for steady-state fusion [J]. Physical Review
Letters, 2019, 122(25): 255001.
[7] NAZIKIAN R, PETTY C C,
BORTOLON A, et al. Grassy-ELM regime with edge resonant magnetic perturbations
in fully noninductive plasmas in the DIII-D tokamaka [J]. Nuclear Fusion, 2018,
58(10): 106010.
[8] YE Y, XU G S, WANG Y F, et al.
Experimental study on low recycling no-ELM high confinement mode in EAST [J].
Nuclear Fusion, 2019, 59(8): 086044.
[9] SNYDER P B, WILSON H R, FERRON
J R, et al. Edge localized modes and the pedestal: A model based on coupled
peeling-ballooning modes [J]. Physics of Plasmas, 2002, 9(5): 2037-2043.
[10] WILSON H R, SNYDER P B,
HUYSMANS G T A, et al. Numerical studies of edge localized instabilities in
tokamaks [J]. Physics of Plasmas, 2002, 9(4): 1277-1286.
[11] FRASSINETTI L, BEURSKENS M N
A, SAARELMA S, et al. Global and pedestal confinement and pedestal structure in
dimensionless collisionality scans of low-triangularity H-mode plasmas in
JET-ILW [J]. Nuclear Fusion, 2016, 57(1): 016012.
[12] SAUTER O, ANGIONI C, LIN-LIU Y
R. Neoclassical conductivity and bootstrap current formulas for general axisymmetric
equilibria and arbitrary collisionality regime [J]. Physics of Plasmas, 1999,
6(7): 2834-2839.
[13] LI G Q, REN Q L, QIAN J P, et
al. Kinetic equilibrium reconstruction on EAST tokamak [J]. Plasma Physics and
Controlled Fusion, 2013, 55(12): 125008.
[14] ISAVNIN A, KILPUA E K J,
KOSKINEN H E J. Grad-Shafranov reconstruction of magnetic clouds: overview and
improvements [J]. Solar Physics, 2011, 273: 205-219.
[15] SNYDER P B, WILSON H R. Ideal magneto
hydrodynamic constraints on the pedestal temperature in tokamaks [J]. Plasma
Physics and Controlled Fusion, 2003, 45(9): 1671.
[16] ROBERTS K V, TAYLOR J B. Magneto
hydrodynamic equations for finite Larmor radius [J]. Physical Review Letters,
1962, 8(5): 197.
[17] OYAMA N, KOJIMA A, AIBA N,
et al. Effects of edge collisionality on ELM characteristics in the grassy ELM
regime [J]. Nuclear Fusion, 2010, 50(6): 064014.
|
