Nonlinear saturation of collisionless trapped electron mode turbulence: Zonal flows and zonal density

2008 ◽  
Vol 15 (5) ◽  
pp. 055907 ◽  
Author(s):  
Jianying Lang ◽  
Scott E. Parker ◽  
Yang Chen
2009 ◽  
Vol 16 (5) ◽  
pp. 055906 ◽  
Author(s):  
D. R. Ernst ◽  
J. Lang ◽  
W. M. Nevins ◽  
M. Hoffman ◽  
Y. Chen ◽  
...  

2005 ◽  
Vol 12 (7) ◽  
pp. 072309 ◽  
Author(s):  
Tilman Dannert ◽  
Frank Jenko

Author(s):  
shuyu Zheng ◽  
Debing Zhang ◽  
Erbing Xue ◽  
Limin Yu ◽  
Xianmei Zhang ◽  
...  

Abstract High poloidal beta scenarios with favorable energy confinement (β_p~1.9, H_98y2~1.4) have been achieved on Experimental Advanced Superconducting Tokamak (EAST) using only radio frequency waves heating. Gyrokinetic simulations are carried out with experimental plasma parameters and tokamak equilibrium data of a typical high β_p discharge by the GTC code. Linear simulations show that electron temperature scale length and electron density scale length destabilize the turbulence, collision effects stabilize the turbulence, and the instability propagates in the electron diamagnetic direction. These indicate that the dominant instability in the core of high β_p plasma is collisionless trapped electron mode. Ion thermal diffusivities calculated by nonlinear gyrokinetic simulations are consistent with the experimental value, in which the electron collision effects play an important role. Further analyses show that instabilities with k_θ ρ_s>0.38 are suppressed by collision effects and collision effects reduce the radial correlation length of turbulence, resulting in the suppression of the turbulence.


2020 ◽  
Vol 86 (3) ◽  
Author(s):  
A. Biancalani ◽  
A. Bottino ◽  
P. Lauber ◽  
A. Mishchenko ◽  
F. Vannini

Numerical simulations of Alfvén modes driven by energetic particles are performed with the gyrokinetic (GK) global particle-in-cell code ORB5. A reversed shear equilibrium magnetic field is adopted. A simplified configuration with circular flux surfaces and large aspect ratio is considered. The nonlinear saturation of beta-induced Alfvén eigenmodes (BAE) is investigated. The roles of the wave–particle nonlinearity of the different species, i.e. thermal ions, electrons and energetic ions are described, in particular for their role in the saturation of the BAE and the generation of zonal flows. The nonlinear redistribution of the electron population is found to be important in increasing the BAE saturation level and the zonal flow amplitude.


2014 ◽  
Vol 21 (5) ◽  
pp. 052306 ◽  
Author(s):  
Y. Asahi ◽  
A. Ishizawa ◽  
T.-H. Watanabe ◽  
H. Tsutsui ◽  
S. Tsuji-Iio

2016 ◽  
Vol 23 (4) ◽  
pp. 042309 ◽  
Author(s):  
Lu Wang ◽  
Shuitao Peng ◽  
P. H. Diamond

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