A Particle Module for the PLUTO Code: I - an implementation of the MHD-PIC equations

TL;DR

This paper introduces a hybrid MHD-PIC module for the PLUTO code, enabling the simulation of cosmic ray effects on plasma dynamics efficiently by combining fluid and kinetic approaches with advanced numerical schemes.

Contribution

It presents a fully conservative, second-order accurate hybrid MHD-PIC implementation with novel sub-cycling for relativistic particles, extending plasma simulation capabilities.

Findings

Successfully models cosmic ray feedback on plasma dynamics.

Demonstrates efficiency gains over traditional PIC simulations.

Validates the module with benchmarks like Bell instability and shock acceleration.

Abstract

We describe an implementation of a particle physics module available for the PLUTO code, appropriate for the dynamical evolution of a plasma consisting of a thermal fluid and a non-thermal component represented by relativistic charged particles, or cosmic rays (CR). While the fluid is approached using standard numerical schemes for magnetohydrodynamics, CR particles are treated kinetically using conventional Particle-In-Cell (PIC) techniques. The module can be used to describe either test particles motion in the fluid electromagnetic field or to solve the fully coupled MHD-PIC system of equations with particle backreaction on the fluid as originally introduced by \cite{Bai_etal.2015}. Particle backreaction on the fluid is included in the form of momentum-energy feedback and by introducing the CR-induced Hall term in Ohm's law. The hybrid MHD-PIC module can be employed to study CR kinetic effects on scales larger than the (ion) skin depth provided the Larmor gyration scale is properly resolved. When applicable, this formulation avoids to resolve microscopic scales offering a substantial computational saving with respect to PIC simulations. We present a fully-conservative formulation which is second-order accurate in time and space and extends to either Runge-Kutta (RK) or corner-transport-upwind (CTU) time-stepping schemes (for the fluid) while a standard Boris integrator is employed for the particles. For highly-energetic relativistic CRs and in order to overcome the time step restriction a novel sub-cycling strategy that retains second-order accuracy in time is presented. Numerical benchmarks and applications including Bell instability, diffusive shock acceleration and test particle acceleration in reconnecting layers are discussed.