On demand triggering of edge localized instabilities using external nonaxisymmetric magnetic perturbations in toroidal plasmas.
暂无分享,去创建一个
T E Evans | J. Manickam | R. Bell | T. Osborne | T. Evans | E. Unterberg | P. Snyder | S. Gerhardt | H. Kugel | J. Park | S. Sabbagh | J. Menard | R. Maingi | J. Canik | S. Paul | R Maingi | J-K Park | S P Gerhardt | T H Osborne | B P Leblanc | R E Bell | J Manickam | P B Snyder | J E Menard | H W Kugel | S A Sabbagh | J M Canik | S F Paul | E A Unterberg | B. LeBlanc
[1] M. Viola,et al. Exploration of spherical torus physics in the NSTX device , 2000 .
[2] L. Zakharov,et al. Transition to ELM-free improved H-mode by lithium deposition on NSTX graphite divertor surfaces , 2009 .
[3] J. S. deGrassie,et al. RMP ELM suppression in DIII-D plasmas with ITER similar shapes and collisionalities , 2008 .
[4] B. Chirikov. A universal instability of many-dimensional oscillator systems , 1979 .
[5] H. Zohm. Edge localized modes (ELMs) , 1996 .
[6] M E Fenstermacher,et al. Suppression of large edge-localized modes in high-confinement DIII-D plasmas with a stochastic magnetic boundary. , 2004, Physical review letters.
[7] A. Hubbard,et al. Studies of EDA H-Mode in Alcator C-Mod , 2000 .
[8] L. Lao,et al. Edge localized modes and the pedestal: A model based on coupled peeling–ballooning modes , 2002 .
[9] J. Manickam,et al. ELM destabilization by externally applied non-axisymmetric magnetic perturbations in NSTX , 2010 .
[10] A. Hyatt,et al. Effects of ergodization on plasma confinement in JFT-2M , 1992 .
[11] A. Boozer,et al. Computation of three-dimensional tokamak and spherical torus equilibria , 2007 .
[12] N Hawkes,et al. Active control of type-I edge-localized modes with n=1 perturbation fields in the JET tokamak. , 2007, Physical review letters.
[13] T. Osborne,et al. Suppression of type-I ELMs using a single toroidal row of magnetic field perturbation coils in DIII-D , 2008 .
[14] T. Osborne,et al. Edge stability of stationary ELM-suppressed regimes on DIII-D , 2008 .
[15] K. Shaing. Magnetohydrodynamic-activity-induced toroidal momentum dissipation in collisionless regimes in tokamaks , 2003 .
[16] R. J. Groebner,et al. Scaling studies of the high mode pedestal , 1998 .
[17] K. Tritz,et al. Observation of a high performance operating regime with small edge-localized modes in the National Spherical Torus Experiment , 2004 .
[18] R. Fitzpatrick. Bifurcated states of a rotating tokamak plasma in the presence of a static error-field , 1998 .
[19] J. S. deGrassie,et al. Effect of island overlap on edge localized mode suppression by resonant magnetic perturbations in DIII-D , 2008 .
[20] John L. Johnson,et al. Computation of the Magnetohydrodynamic Spectrum in Axisymmetric Toroidal Confinement Systems , 1976 .
[21] M. Ono,et al. The effect of lithium surface coatings on plasma performance in the National Spherical Torus Experiment , 2008 .
[22] K. Tritz,et al. Active stabilization of the resistive-wall mode in high-beta, low-rotation plasmas. , 2006, Physical review letters.
[23] R. Bell,et al. Observation of plasma toroidal-momentum dissipation by neoclassical toroidal viscosity. , 2006, Physical review letters.
[24] T. L. Rhodes,et al. Suppression of large edge localized modes with edge resonant magnetic fields in high confinement DIII-D plasmas , 2005 .
[25] Lao,et al. Regime of very high confinement in the boronized DIII-D tokamak. , 1991, Physical review letters.
[26] D K Mansfield,et al. Edge-localized-mode suppression through density-profile modification with lithium-wall coatings in the National Spherical Torus Experiment. , 2009, Physical review letters.
[27] L. Lao,et al. Quiescent double barrier high-confinement mode plasmas in the DIII-D tokamak , 2001 .