Electron Heating in 2D Particle-in-Cell Simulations of Quasi-Perpendicular Low-Beta Shocks
arXiv:2308.16462 · doi:10.3847/1538-4357/ad1f69
Abstract
We measure the thermal electron energization in 1D and 2D particle-in-cell (PIC) simulations of quasi-perpendicular, low-beta () collisionless ion-electron shocks with mass ratio , fast Mach number -, and upstream magnetic field angle - from shock normal . It is known that shock electron heating is described by an ambipolar, -parallel electric potential jump, , that scales roughly linearly with the electron temperature jump. Our simulations have - in units of the pre-shock ions' bulk kinetic energy, in agreement with prior measurements and simulations. Different ways to measure , including the use of de Hoffmann-Teller frame fields, agree to tens-of-percent accuracy. Neglecting off-diagonal electron pressure tensor terms can lead to a systematic underestimate of in our low- shocks. We further focus on two shocks: a () case with a long, precursor of whistler waves along , and a () case with a shorter, precursor of whistlers oblique to both and ; is the ion skin depth. Within the precursors, has a secular rise towards the shock along multiple whistler wavelengths and also has localized spikes within magnetic troughs. In a 1D simulation of the , case, shows a weak dependence on the electron plasma-to-cyclotron frequency ratio , and decreases by a factor of 2 as is raised to the true proton-electron value of 1836.
arXiv comment32 pages, 25 figures; accepted to ApJ. Figures 6, 8, 16, 23 updated to fix Liouville mapping procedure normalization (Equation (8))
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