scholarly journals Nonlinear dynamics of energetic-particle driven geodesic acoustic modes in ASDEX Upgrade

2020 ◽  
Vol 27 (4) ◽  
pp. 042512 ◽  
Author(s):  
I. Novikau ◽  
A. Biancalani ◽  
A. Bottino ◽  
Ph. Lauber ◽  
E. Poli ◽  
...  
2017 ◽  
Vol 83 (6) ◽  
Author(s):  
A. Biancalani ◽  
I. Chavdarovski ◽  
Z. Qiu ◽  
A. Bottino ◽  
D. Del Sarto ◽  
...  

The nonlinear dynamics of energetic-particle (EP) driven geodesic acoustic modes (EGAM) is investigated here. A numerical analysis with the global gyrokinetic particle-in-cell code ORB5 is performed, and the results are interpreted with the analytical theory, in close comparison with the theory of the beam-plasma instability. Only axisymmetric modes are considered, with a nonlinear dynamics determined by wave–particle interaction. Quadratic scalings of the saturated electric field with respect to the linear growth rate are found for the case of interest. As a main result, the formula for the saturation level is provided. Near the saturation, we observe a transition from adiabatic to non-adiabatic dynamics, i.e. the frequency chirping rate becomes comparable to the resonant EP bounce frequency. The numerical analysis is performed here with electrostatic simulations with circular flux surfaces, and kinetic effects of the electrons are neglected.


2018 ◽  
Vol 84 (6) ◽  
Author(s):  
A. Biancalani ◽  
N. Carlevaro ◽  
A. Bottino ◽  
G. Montani ◽  
Z. Qiu

The nonlinear dynamics of energetic-particle (EP) driven geodesic acoustic modes (EGAM) in tokamaks is investigated, and compared with the beam-plasma system (BPS). The EGAM is studied with the global gyrokinetic (GK) particle-in-cell code ORB5, treating the thermal ions and EP (in this case, fast ions) as GK and neglecting the kinetic effects of the electrons. The wave–particle nonlinearity is only considered in the EGAM nonlinear dynamics. The BPS is studied with a one-dimensional code where the thermal plasma is treated as a linear dielectric, and the EP (in this case, fast electrons) with an N-body Hamiltonian formulation. A one-to-one mapping between the EGAM and the BPS is described. The focus is on understanding and predicting the EP redistribution in phase space. We identify here two distinct regimes for the mapping: in the low-drive regime, the BPS mapping with the EGAM is found to be complete, and in the high-drive regime, the EGAM dynamics and the BPS dynamics are found to differ. The transition is described with the presence of a non-negligible frequency chirping, which affects the EGAM but not the BPS, above the identified drive threshold. The difference can be resolved by adding an ad hoc frequency modification to the BPS model. As a main result, the formula for the prediction of the nonlinear width of the velocity redistribution around the resonance velocity is provided. This article is written as the second of a series of articles (the first being Biancalani et al. (J. Plasma Phys., vol. 83 (6), 2017, 725830602)) on the saturation of EGAMs due to wave–particle nonlinearity.


2016 ◽  
Vol 23 (10) ◽  
pp. 102501 ◽  
Author(s):  
M. Sasaki ◽  
N. Kasuya ◽  
K. Itoh ◽  
K. Hallatschek ◽  
M. Lesur ◽  
...  

2018 ◽  
Vol 13 (0) ◽  
pp. 3403040-3403040
Author(s):  
Makoto SASAKI ◽  
Kimitaka ITOH ◽  
Takeshi IDO ◽  
Akihiro SHIMIZU ◽  
Tatsuya KOBAYASHI ◽  
...  

2018 ◽  
Vol 58 (10) ◽  
pp. 106030 ◽  
Author(s):  
D. Zarzoso ◽  
D. del-Castillo-Negrete ◽  
D.F. Escande ◽  
Y. Sarazin ◽  
X. Garbet ◽  
...  

2017 ◽  
Vol 7 (1) ◽  
Author(s):  
M. Sasaki ◽  
K. Itoh ◽  
K. Hallatschek ◽  
N. Kasuya ◽  
M. Lesur ◽  
...  

Author(s):  
Li-Ming Yu ◽  
Fulvio Zonca ◽  
Zhiyong Qiu ◽  
Liu Chen ◽  
Wei Chen ◽  
...  

Abstract Recent observations in HL-2A tokamak give new experimental evidences of energetic particle mode (EPM) avalanche. In a strong EPM burst, the mode structure propagates radially outward within two hundred Alfvén time, while the frequency of the dominant mode changes self-consistently to maximize wave-particle power exchange and mode growth. This suggests that significant energetic particle transport occurs in this avalanche phase, in agreement with theoretical framework of EPM convective amplification. A simplified relay runner model yields satisfactory interpretations of the measurements. The results can help understanding the nonlinear dynamics of energetic particle driven modes in future burning plasmas, such as ITER.


2012 ◽  
Vol 52 (12) ◽  
pp. 123015 ◽  
Author(s):  
R.K. Fisher ◽  
D.C. Pace ◽  
G.J. Kramer ◽  
M.A. Van Zeeland ◽  
R. Nazikian ◽  
...  

2013 ◽  
Vol 110 (12) ◽  
Author(s):  
D. Zarzoso ◽  
Y. Sarazin ◽  
X. Garbet ◽  
R. Dumont ◽  
A. Strugarek ◽  
...  

2021 ◽  
Vol 87 (4) ◽  
Author(s):  
I. Chavdarovski ◽  
M. Schneller ◽  
A. Biancalani

We derive the local dispersion relation of energetic-particle-induced geodesic acoustic modes (EGAMs) for both trapped and circulating ion beams with single pitch angle slowing-down and Maxwellian distributions, as well as a bump-on-tail distribution in tokamak plasmas. For slowing-down and Maxwellian particles, the solutions of the local dispersion relation give the spectrum, growth rate and thresholds of excitation as functions of the pitch angle, beam density and frequency of the energetic particles bounce motion. For circulating ions there is only one unstable branch with frequency below the GAM continuum and a threshold of excitation in the pitch angle, for both the slowing-down and single pitch Maxwellian distributions. Trapped particles cause no excitation of a mode for neither slowing-down nor Maxwellian ion beams, but they can excite a mode with a bump-on-tail distribution when the mean velocity of the beam is larger than the threshold and the energetic particle bounce frequency is high enough.


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