Magnetic Field Saturation of the Ion Weibel Instability in Interpenetrating Relativistic Plasmas
arXiv:1805.07188 · doi:10.3847/2041-8213/aac6d6
Abstract
The time evolution and saturation of the Weibel instability at the ion Alfvén current are presented by ab initio particle-in-cell simulations. We found that the ion Weibel current in 3D could evolve into the Alfvén current where the magnetic field energy is sustained at 1.5\% of the initial beam kinetic energy. The current filaments are no longer isolated at saturation, but rather connected to each other to form a network structure. Electrons are continuously heated during the coalescence of the filaments, which is crucial for obtaining sustained magnetic fields with much stronger levels than with 2D simulations. The results highlight again the importance of the Weibel instability in generating magnetic fields in laboratory, astrophysical, and cosmological situations.
arXiv comment4 pages, 4 figures, accepted for publication in ApJL
References in corpus (23)
- Gamma-Ray Bursts and the Fireball Model
- Evidence for a Canonical GRB Afterglow Light Curve in the Swift/XRT Data
- Generation of Magnetic Fields in the Relativistic Shock of Gamma-Ray-Burst Sources
- The Maximum Energy of Accelerated Particles in Relativistic Collisionless Shocks
- On the structure of relativistic collisionless shocks in electron-ion plasmas
- Observation of magnetic field generation via the Weibel instability in interpenetrating plasma flows
- Magnetic fields and spiral arms in the galaxy M51
- The surprising Crab pulsar and its nebula: A review
- Magnetic Field Generation in Collisionless Shocks; Pattern Growth and Transport
- Relativistic Shocks: Particle Acceleration and Magnetization
- Filamentation instability of counter-streaming laser-driven plasmas
- Non-relativistic Collisionless Shocks in Unmagnetized Electron-Ion Plasmas
- Weibel, Two-Stream, Filamentation, Oblique, Bell, Buneman... which one grows faster ?
- Non-Fermi Power law Acceleration in Astrophysical Plasma Shocks
- Saturation mechanism of the Weibel instability in weakly magnetized plasmas
- Electron Surfing and Drift Accelerations in a Weibel-dominated High-Mach-number Shock
- Cluster magnetic fields from large-scale-structure and galaxy-cluster shocks
- Relativistic Collisionless Shocks in Unmagnetized Electron-Positron Plasmas
- Production of magnetic energy by macroscopic turbulence in GRB afterglows
- 3D modeling of collisionless shocks
- Nonlinear dynamics of the ion Weibel-filamentation instability: an analytical model for the evolution of the plasma and spectral properties
- Stability Property of Numerical Cherenkov Radiation and its Application to Relativistic Shock Simulations
- Weibel instability driven by spatially anisotropic density structures
Cited by in corpus (14)
- Constraining the magnetic field structure in collisionless relativistic shocks with a radio afterglow polarization upper limit in GW170817
- Long-term Evolution of Relativistic Unmagnetized Collisionless Shocks
- Weibel-Mediated Shocks Propagating into Inhomogeneous Electron-Positron Plasmas
- Temperature-dependent Saturation of Weibel-type Instabilities in Counter-streaming Plasmas
- Microphysics of Relativistic Collisionless Electron-ion-positron Shocks
- Origin and Impacts of the First Cosmic Rays
- Noise-Induced Magnetic Field Saturation in Kinetic Simulations
- Enhanced Magnetic Field Amplification by Ion-Beam Weibel Instability in Weakly Magnetized Astrophysical Shocks
- Synchrotron Polarization of Gamma-Ray Burst Afterglow Shocks with Hydrodynamic-scale Turbulent Magnetic Field
- Saturation of the asymmetric current filamentation instability under conditions relevant to relativistic shock precursors
- Saturation Level of Ion Weibel Instability and Isotropization Length Scale in Electron-Ion Weibel-Mediated Shocks
- Evolution of three-dimensional Relativistic Ion Weibel Instability: Competition with Kink Instability
- Energy partition in collisionless counterstreaming plasmas
- The most distant optically polarised GRB afterglow: GRB 240419A at z = 5.178