Particle acceleration in a reconnecting current sheet: PIC simulation

TL;DR

This study uses 2D3V PIC simulations to investigate proton and electron acceleration in a reconnecting current sheet, revealing the significant role of polarization electric fields and guiding fields in particle trajectories and energy distributions.

Contribution

It demonstrates the impact of polarization electric fields on particle acceleration and ejection, providing new insights beyond test particle approaches in reconnecting current sheets.

Findings

Polarization electric field influences particle trajectories and ejection asymmetry.

Electrons and protons are ejected into the same semispace due to the polarization field.

Electron energy distribution is wide and single-peaked, differing from test particle predictions.

Abstract

The acceleration of protons and electrons in a reconnecting current sheet (RCS) is simulated with a particle-in-cell (PIC) 2D3V code for the proton-to-electron mass ratio of 100. The electro-magnetic configuration forming the RCS incorporates all three components of the magnetic field (including the guiding field) and a drifted electric field. PIC simulations reveal that there is a polarisation electric field that appears during acceleration owing to a separation of electrons from protons towards the midplane of the RCS. If the plasma density is low, the polarisation field is weak and the particle trajectories in the PIC simulations are similar to those in the test particle (TP) approach. For the higher plasma density the polarisation field is stronger and it affects the trajectories of protons by increasing their orbits during acceleration. This field also leads to a less asymmetrical abundances of ejected protons towards the midplane in comparison with the TP approach. For a given magnetic topology electrons in PIC simulations are ejected to the same semispace as protons, contrary to the TP results. This happens because the polarisation field extends far beyond the thickness of a current sheet. This field decelerates the electrons, which are initially ejected into the semispace opposite to the protons, returns them back to the RCS, and, eventually, leads to the electron ejection into the same semispace as protons. Energy distribution of the ejected electrons is rather wide and single-peak, contrary to the two-peak narrow-energy distribution obtained in the TP approach. In the case of a strong guiding field, the mean energy of the ejected electrons is found to be smaller than it is predicted analytically and by the TP simulations.