scholarly journals E × B electron drift instability in Hall thrusters: Particle-in-cell simulations vs. theory

2018 ◽  
Vol 25 (6) ◽  
pp. 061204 ◽  
Author(s):  
J. P. Boeuf ◽  
L. Garrigues
2019 ◽  
Vol 28 (6) ◽  
pp. 064002 ◽  
Author(s):  
Francesco Taccogna ◽  
Pierpaolo Minelli ◽  
Zahra Asadi ◽  
Guillaume Bogopolsky

2006 ◽  
Vol 13 (10) ◽  
pp. 102111 ◽  
Author(s):  
A. Ducrocq ◽  
J. C. Adam ◽  
A. Héron ◽  
G. Laval

2018 ◽  
Vol 25 (6) ◽  
pp. 063522 ◽  
Author(s):  
Vivien Croes ◽  
Antoine Tavant ◽  
Romain Lucken ◽  
Roberto Martorelli ◽  
Trevor Lafleur ◽  
...  

2021 ◽  
Vol 145 ◽  
pp. 110810
Author(s):  
D. Mandal ◽  
Y. Elskens ◽  
X. Leoncini ◽  
N. Lemoine ◽  
F. Doveil

2021 ◽  
Author(s):  
Zhongwei Yang ◽  
Shuichi Matsukiyo ◽  
Huasheng Xie ◽  
Fan Guo ◽  
Mingzhe Liu ◽  
...  

<p><span>Microinstabilities and waves excited at perpendicular interplanetary shocks in the near-Sun solar wind are investigated by full particle-in-cell simulations. By analyzing the dispersion relation of fluctuating field components directly issued from the shock simulation, we obtain key findings concerning wave excitations at the shock front: (1) at the leading edge of the foot, two types of electrostatic (ES) waves are observed. The relative drift of the reflected ions versus the electrons triggers an electron cyclotron drift instability (ECDI) that excites the first ES wave. Because the bulk velocity of gyro-reflected ions shifts to the direction of the shock front, the resulting ES wave propagates obliquely to the shock normal. Immediately, a fraction of incident electrons are accelerated by this ES wave and a ring-like velocity distribution is generated. They can couple with the hot Maxwellian core and excite the second ES wave around the upper hybrid frequency. (2) From the middle of the foot all the way to the ramp, electrons can couple with both incident and reflected ions. ES waves excited by ECDI in different directions propagate across each other. Electromagnetic (EM) waves (X mode) emitted toward upstream are observed in both regions. They are probably induced by a small fraction of relativistic electrons. The impact of shock front rippling, Mach numbers, and dimensions on the ES wave excitation also will be discussed. Results shed new insight on the mechanism for the occurrence of ES wave excitations and possible EM wave emissions at young coronal mass ejection–driven shocks in the near-Sun solar wind.</span></p>


1979 ◽  
Vol 22 (4) ◽  
pp. 669 ◽  
Author(s):  
Swadesh M. Mahajan ◽  
David W. Ross

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