The MHD-kinetic hybrid code MEGA is used to analyze the stability of beam-driven JT-60SA ramp-up plasmas with respect to nonresonant and resonant instabilities. Mode structures, growth rates, saturation levels and modifications of the plasma profiles are computed for several cases. The observations are interpreted using MHD stability criteria and orbit-based resonance analysis. It is concluded that the integrated code TOPICS-BAFP should include a model for multiple tearing modes, since these have the largest effect in our simulations.3rd UNIST-Kyoto Univ. Workshop on “Physics validation and control of turbulent transport and MHD in fusion plasmas
Long-pulse plasma operation at high normalized beta, beta(N), above the n = 1 ideal MHD no-wall stab...
The development of methods for the active control of magnetohydrodynamic (MHD) instabilities and the...
The superconducting tokamak JT-60SA is being built in Naka (Japan) under the Broader Approach Satell...
The MHD-kinetic hybrid code MEGA is used to analyze the stability of beam-driven JT-60SA ramp-up pla...
A beam-driven ramp-up scenario for JT-60SA is analyzed with respect to stability of pressure- and cu...
The hybrid code MEGA is used to study the excitation of MHD ballooning, double tearing, and fast-ion...
We report results of global resistive magnetohydrodynamic (MHD) simulations, which predict that wide...
The hybrid code MEGA has been used to study the ramp-up phase of a high-beta plasma in the JT-60SA t...
We analyze the effects of the passing energetic particles on the resistive ballooning modes (RBM) an...
The stability with respect to a peeling–ballooning mode (PBM) was investigated numerically with exte...
The hybrid code MEGA developed at NIFS/Japan is now playing a world-leading role in energetic partic...
The superconducting tokamak JT-60SA is being built in Naka (Japan) under the Broader Approach Satell...
The superconducting tokamak JT-60SA is being built in Naka (Japan) under the Broader Approach Satell...
Long-pulse plasma operation at high normalized beta, beta(N), above the n = 1 ideal MHD no-wall stab...
The development of methods for the active control of magnetohydrodynamic (MHD) instabilities and the...
The superconducting tokamak JT-60SA is being built in Naka (Japan) under the Broader Approach Satell...
The MHD-kinetic hybrid code MEGA is used to analyze the stability of beam-driven JT-60SA ramp-up pla...
A beam-driven ramp-up scenario for JT-60SA is analyzed with respect to stability of pressure- and cu...
The hybrid code MEGA is used to study the excitation of MHD ballooning, double tearing, and fast-ion...
We report results of global resistive magnetohydrodynamic (MHD) simulations, which predict that wide...
The hybrid code MEGA has been used to study the ramp-up phase of a high-beta plasma in the JT-60SA t...
We analyze the effects of the passing energetic particles on the resistive ballooning modes (RBM) an...
The stability with respect to a peeling–ballooning mode (PBM) was investigated numerically with exte...
The hybrid code MEGA developed at NIFS/Japan is now playing a world-leading role in energetic partic...
The superconducting tokamak JT-60SA is being built in Naka (Japan) under the Broader Approach Satell...
The superconducting tokamak JT-60SA is being built in Naka (Japan) under the Broader Approach Satell...
Long-pulse plasma operation at high normalized beta, beta(N), above the n = 1 ideal MHD no-wall stab...
The development of methods for the active control of magnetohydrodynamic (MHD) instabilities and the...
The superconducting tokamak JT-60SA is being built in Naka (Japan) under the Broader Approach Satell...