scholarly journals Energy-conserving time propagation for a structure-preserving particle-in-cell Vlasov–Maxwell solver

2021 ◽  
Vol 425 ◽  
pp. 109890
Author(s):  
Katharina Kormann ◽  
Eric Sonnendrücker
2019 ◽  
Vol 236 ◽  
pp. 153-163 ◽  
Author(s):  
Diego Gonzalez-Herrero ◽  
Alfredo Micera ◽  
Elisabetta Boella ◽  
Jaeyoung Park ◽  
Giovanni Lapenta

2014 ◽  
Vol 32 (3) ◽  
pp. 399-407 ◽  
Author(s):  
Mohammad Ghorbanalilu ◽  
Elahe Abdollahzadeh ◽  
S.H. Ebrahimnazhad Rahbari

AbstractWe have performed extensive one dimensional particle-in-cell (PIC) simulations to explore generation of electrostatic waves driven by two-stream instability (TSI) that arises due to the interaction between two symmetric counterstreaming electron beams. The electron beams are considered to be cold, collisionless and magnetic-field-free in the presence of neutralizing background of static ions. Here, electrons are described by the non-extensive q-distributions of the Tsallis statistics. Results shows that the electron holes structures are different for various q values such that: (i) for q > 1 cavitation of electron holes are more visible and the excited waves were more strong (ii) for q < 1 the degree of cavitation decreases and for q = 0.5 the holes are not distinguishable. Furthermore, time development of the velocity root-mean-square (VRMS) of electrons for different q-values demonstrate that the maximum energy conversion is increased upon increasing the non-extensivity parameter q up to the values q > 1. The normalized total energy history for a arbitrary entropic index q = 1.5, approves the energy conserving in our PIC simulation.


2017 ◽  
Vol 83 (2) ◽  
Author(s):  
Giovanni Lapenta ◽  
Diego Gonzalez-Herrero ◽  
Elisabetta Boella

The recently developed energy conserving semi-implicit method (ECsim) for particle-in-cell (PIC) simulation is applied to multiple-scale problems where the electron-scale physics needs to be only partially retained and the interest is on the macroscopic or ion-scale processes. Unlike hybrid methods, the ECsim is capable of providing kinetic electron information, such as wave–electron interaction (Landau damping or cyclotron resonance) and non-Maxwellian electron velocity distributions. However, like hybrid methods, the ECsim does not need to resolve all electron scales, allowing time steps and grid spacings orders of magnitude larger than in explicit PIC schemes. The additional advantage of the ECsim is that the stability at large scale is obtained while conserving energy exactly. Three examples are presented: ion acoustic waves, electron acoustic instability and reconnection processes.


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