Abstract

Strong shear flow regions found in astrophysical jets are shown to be important dissipation regions, where the shear flow kinetic energy flow is converted into electric and magnetic field energy via shear instabilities. The emergence of these self-consistent fields makes shear flows significant sites for radiation emission and particle acceleration. We focus on electron-scale instabilities, namely the collisionless, unmagnetized electron-scale Kelvin–Helmholtz instability (ESKHI) and a large-scale DC magnetic field generation mechanism on the electron scales. We show that these processes are important candidates to generate magnetic fields in the presence of strong velocity shears, which may naturally originate in energetic matter outbursts of active galactic nuclei and gamma-ray bursters. We show that the ESKHI is robust to density jumps between shearing flows, thus operating in various scenarios with different density contrasts. Multidimensional particle-in-cell (PIC) simulations of the ESKHI, performed with OSIRIS, reveal the emergence of a strong and large-scale DC magnetic field component, which is not captured by the standard linear fluid theory. This DC component arises from kinetic effects associated with the thermal expansion of electrons of one flow into the other across the shear layer, whilst ions remain unperturbed due to their inertia. The electron expansion forms DC current sheets, which induce a DC magnetic field. Our results indicate that most of the electromagnetic energy developed in the ESKHI is stored in the DC component, reaching values of equipartition on the order of in the electron time-scale, and persists longer than the proton time-scale. Particle scattering/acceleration in the self-generated fields of these shear flow instabilities is also analyzed.

Highlights

  • Relativistic jets are found in a wide range of extreme astrophysical scenarios like active galactic nuclei (AGN) and gamma-ray bursts (GRBs) (Bridle 1984, Mirabel and Rodriguez 1999)

  • Shear instabilities in plasmas are usually studied within the framework of magnetohydrodynamics, where the plasma is considered as a magnetized fluid and where the typical time scale is governed by ion motion

  • We have shown in this work that electron-scale physics leads to a variety of new effects when one considers an initially unmagnetized cold shearing collisionless plasma

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Summary

Introduction

Relativistic jets are found in a wide range of extreme astrophysical scenarios like active galactic nuclei (AGN) and gamma-ray bursts (GRBs) (Bridle 1984, Mirabel and Rodriguez 1999). External shear layers, resulting from the interaction of the jet with the interstellar medium, may be considered In these scenarios, collisionless shear instabilities such as the Kelvin–Helmholtz instability (KHI) at the MHD scale (D’Angelo 1965) or at even shorter scales (Gruzinov 2008, Zhang et al 2009) play a role in the dissipation of the jet kinetic energy into electric and magnetic turbulence (Alves et al 2012, Liang et al 2013, Zhang et al 2009). The KHI in charged fluids (plasmas) has been studied within the MHD framework (D’Angelo 1965, Thomas and Winske 1991), where the shearing flows interact via electric and magnetic fields, in addition to pressure gradients In both these frameworks, the length (and time) scales involved are much larger than the kinetic scales associated with the particles that make up the neutral or charged fluid. The theoretical results are compared and verified with PIC simulations

Linear two-fluid theory
Comparisons with PIC simulations
Finite velocity shear gradient
DC magnetic field generation in unmagnetized shear flows
Warm shear flow
Cold shear flow
Particle acceleration
Conclusions
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