A new Particle-in-Cell (PIC) method, that conserves energy exactly, is pre-sented. The particle equations of motion and the Maxwell’s equations are differenced implicitly in time by the midpoint rule and solved concurrently by a Jacobian-free Newton Krylov (JFNK) solver. Several tests show that the finite grid instability is eliminated in energy conserving PIC simulations, and the method correctly describes the two-stream and Weibel instabilities, conserving exactly the total energy. The computational time of the energy conserving PIC method increases linearly with the number of particles, and it is rather insensitive to the number of grid points and time step. The kinetic enslavement technique can be effectively used to reduce the problem ...
International audienceThis work presents new parallelizable numerical schemes for the integration of...
In this paper, we develop an asymptotic-preserving and energy-conserving (APEC) Particle-In-Cell (PI...
It is shown that a simple algorithm which exactly segregates between adiabatic and non-adiabatic ele...
Most current particle-in-cell (PIC) algorithms employ an explicit approach. Explicit PIC approaches ...
This work presents a set of preconditioning strategies able to significantly accelerate the performa...
An algorithm for time reduction is implemented to an existing particle-in-cell (PIC) code to simulat...
PIC (Particle-in-cell) modeling is a computational technique which functions by advancing computer p...
The recently developed energy conserving semi-implicit method (ECsim) for particle-in-cell (PIC) sim...
This paper discusses a novel fully implicit formulation for a one-dimensional electrostatic particle...
We propose a new particle-in-cell (PIC) method for the simulation of plasmas based on a recently dev...
Particle-in-cell merging algorithms aim to resample dynamically the six-dimensional phase space occu...
© 2018 Elsevier B.V. We present in this work the implementation of the Energy Conserving Semi-Implic...
A new scheme, based on an exact separation between adiabatic and nonadiabatic electron responses, fo...
In the integration of the equations of motion of a system of particles, conventional numerical metho...
Figure 1: APIC/PIC blends yield more energetic and more stable behavior than FLIP/PIC blends in a wi...
International audienceThis work presents new parallelizable numerical schemes for the integration of...
In this paper, we develop an asymptotic-preserving and energy-conserving (APEC) Particle-In-Cell (PI...
It is shown that a simple algorithm which exactly segregates between adiabatic and non-adiabatic ele...
Most current particle-in-cell (PIC) algorithms employ an explicit approach. Explicit PIC approaches ...
This work presents a set of preconditioning strategies able to significantly accelerate the performa...
An algorithm for time reduction is implemented to an existing particle-in-cell (PIC) code to simulat...
PIC (Particle-in-cell) modeling is a computational technique which functions by advancing computer p...
The recently developed energy conserving semi-implicit method (ECsim) for particle-in-cell (PIC) sim...
This paper discusses a novel fully implicit formulation for a one-dimensional electrostatic particle...
We propose a new particle-in-cell (PIC) method for the simulation of plasmas based on a recently dev...
Particle-in-cell merging algorithms aim to resample dynamically the six-dimensional phase space occu...
© 2018 Elsevier B.V. We present in this work the implementation of the Energy Conserving Semi-Implic...
A new scheme, based on an exact separation between adiabatic and nonadiabatic electron responses, fo...
In the integration of the equations of motion of a system of particles, conventional numerical metho...
Figure 1: APIC/PIC blends yield more energetic and more stable behavior than FLIP/PIC blends in a wi...
International audienceThis work presents new parallelizable numerical schemes for the integration of...
In this paper, we develop an asymptotic-preserving and energy-conserving (APEC) Particle-In-Cell (PI...
It is shown that a simple algorithm which exactly segregates between adiabatic and non-adiabatic ele...