Particle acceleration in a reconnecting current sheet: PIC simulation

The acceleration of protons and electrons in a reconnecting current sheet (RCS) is simulated with a particle-in-cell (PIC) 2D3V (two-dimensional in space and three-dimensional in velocity spate) code for the proton-to-electron mass ratio of 100 The electromagnetic 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, polarization electric field that appears during acceleration owing to a separation of electrons from protons towards the midplane of the RCS. If Be plasma density is low, the polarization AM 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 polarization field is stronger and it affects the trajectories of protons by increasing their orbits during acceleration. This field also leads to a, less asymmetrical abundance 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, in contrast to the TP results. This happens because the polarization 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. The energy distribution of the ejected electrons is rather wide and single-peaked, in contrast to the two-peak narrow-energy distribution obtained in the TP approach. In the case of a strong guiding field, the the mean energy of the ejected electrons is found to be smaller than it is predicted analytically and by the TP simulations. The beam of accelerated electrons is also found to generate turbulent electric field in the form of Langmuir waves.