During beam injection in the DIII-D tokamak, modes with lower frequencies than expected for toroidicity induced Alfvén eigenmodes (TAEs) are often observed. The experimental 'TAE' frequency is often ≈0.8 of the nominal theoretical frequency of the TAE, fTAE, while the typical frequency of beta induced Alfvén eigenmodes (BAEs) is (0.2-0.4) fTAE. An analysis is presented of an unstable discharge with a high n stability code, HINST, that includes the effect of energetic ions on mode frequency. The analysis shows that the experimental 'TAE' and 'BAE' could be resonant branches of the TAE and the kinetic ballooning mode, respectively
The stability of high-n toroidicity-induced shear Alfven eigenmodes (TAE) in the presence of fusion ...
Global gyrokinetic simulations find that realistic density gradients of energetic particles can simu...
The stability of beta-induced Alfvén eigenmodes (BAE) and the low frequency modes (LFMs) that were f...
During beam injection in the DIII-D tokamak, modes with lower frequencies than expected for toroidic...
A major goal of the DIII-D program is to study 'advanced tokamak' plasmas with good confinement, lar...
Energetic ions can drive Alfvén gap modes unstable, causing large losses of fast ions. Toroidicity-i...
Linear properties of the toroidal Alfvén eigenmode (TAE) excited by energetic particles (EP) in a DI...
The observed characteristics of toroidicity induced Alfven eigenmodes (TAE) in DIII-D tokamak discha...
A summary of fast ion experiments in the DIII-D lokamak is given. Most of the experiments involve ∼8...
Neutral beams were injected into low field (B = 0.7-1.0 T) deuterium plasmas in an attempt to destab...
Linear properties of the toroidal Alfven eigenmode (TAE) excited by energetic particles (EP) in a DI...
Toroidicity induced Alfven eigenmodes (TAE) are observed in the DIII-D tokamak when energetic beam i...
The internal structure of the toroidicity-induced Alfvén eigenmode (TAE) is studied by comparing sof...
Kinetic theory and experimental observations of a special class of energetic particle driven instabi...
An instability with a lower frequency than the toroidicity-induced Alfvén eigenmode was initially id...
The stability of high-n toroidicity-induced shear Alfven eigenmodes (TAE) in the presence of fusion ...
Global gyrokinetic simulations find that realistic density gradients of energetic particles can simu...
The stability of beta-induced Alfvén eigenmodes (BAE) and the low frequency modes (LFMs) that were f...
During beam injection in the DIII-D tokamak, modes with lower frequencies than expected for toroidic...
A major goal of the DIII-D program is to study 'advanced tokamak' plasmas with good confinement, lar...
Energetic ions can drive Alfvén gap modes unstable, causing large losses of fast ions. Toroidicity-i...
Linear properties of the toroidal Alfvén eigenmode (TAE) excited by energetic particles (EP) in a DI...
The observed characteristics of toroidicity induced Alfven eigenmodes (TAE) in DIII-D tokamak discha...
A summary of fast ion experiments in the DIII-D lokamak is given. Most of the experiments involve ∼8...
Neutral beams were injected into low field (B = 0.7-1.0 T) deuterium plasmas in an attempt to destab...
Linear properties of the toroidal Alfven eigenmode (TAE) excited by energetic particles (EP) in a DI...
Toroidicity induced Alfven eigenmodes (TAE) are observed in the DIII-D tokamak when energetic beam i...
The internal structure of the toroidicity-induced Alfvén eigenmode (TAE) is studied by comparing sof...
Kinetic theory and experimental observations of a special class of energetic particle driven instabi...
An instability with a lower frequency than the toroidicity-induced Alfvén eigenmode was initially id...
The stability of high-n toroidicity-induced shear Alfven eigenmodes (TAE) in the presence of fusion ...
Global gyrokinetic simulations find that realistic density gradients of energetic particles can simu...
The stability of beta-induced Alfvén eigenmodes (BAE) and the low frequency modes (LFMs) that were f...