Electrostatic Waves and Electron Holes in Simulations of Low-Mach Quasi-perpendicular Shocks

• Published in: The Astrophysical journal Vol. 974; no. 1; pp. 37 - 54
• Main Authors: Bohdan, Artem, Tran, Aaron, Sironi, Lorenzo, Wilson, Lynn B.
• Format: Journal Article
• Language: English
• Published: Philadelphia The American Astronomical Society 01.10.2024; IOP Publishing
• Subjects: Acoustic waves; Amplitudes; Electric fields; Electron beams; Electrons; Electrostatic waves; Holes (electron deficiencies); Ion beams; LF electric fields; Particle interactions; Planetary bow shocks; Plasma astrophysics; Shocks; Simulation; Solitary waves; Space plasmas; Whistler waves
• ISSN: 0004-637X; 1538-4357
• DOI: 10.3847/1538-4357/ad6b0c

Abstract Collisionless low-Mach-number shocks are abundant in astrophysical and space plasma environments, exhibiting complex wave activity and wave–particle interactions. In this paper, we present 2D Particle-in-Cell (PIC) simulations of quasi-perpendicular nonrelativistic ( v sh ≈ (5500–22000) km s −1 ) low-Mach-number shocks, with a specific focus on studying electrostatic waves in the shock ramp and precursor regions. In these shocks, an ion-scale oblique whistler wave creates a configuration with two hot counterstreaming electron beams, which drive unstable electron acoustic waves (EAWs) that can turn into electrostatic solitary waves (ESWs) at the late stage of their evolution. By conducting simulations with periodic boundaries, we show that the EAW properties agree with linear dispersion analysis. The characteristics of ESWs in shock simulations, including their wavelength and amplitude, depend on the shock velocity. When extrapolated to shocks with realistic velocities ( v sh ≈ 300 km s −1 ), the ESW wavelength is reduced to one-tenth of the electron skin depth and the ESW amplitude is anticipated to surpass that of the quasi-static electric field by more than a factor of 100. These theoretical predictions may explain a discrepancy, between PIC and satellite measurements, in the relative amplitude of high- and low-frequency electric field fluctuations.