A stringent limit on the amplitude of alfvénic perturbations in high-beta low-collisionality plasmas

Journal article

It is shown that low-collisionality plasmas cannot support linearly polarized shear-Alfvén fluctuations above a critical amplitude δB⊥/B0 ∼ B-1/2, where β is the ratio of thermal to magnetic pressure. Above this cutoff, a developing fluctuation will generate a pressure anisotropy that is sufficient to destabilize itself through the parallel firehose instability. This causes the wave frequency to approach zero, interrupting the fluctuation before any oscillation. The magnetic field lines rapidly relax into a sequence of angular zig-zag structures. Such a restrictive bound on shear-Alfvén-wave amplitudes has far-reaching implications for the physics of magnetized turbulence in the high-β conditions prevalent in many astrophysical plasmas, as well as for the solar wind at ∼1 au where β ≳ 1.

Authors: Squire, J; Quataert, E; Schekochihin, A

• Publication status: Published
• Peer review status: Peer reviewed
• Publisher: IOP Publishing
• Journal: Astrophysical Journal Letters
• Volume: 830
• Issue: 2
• Pages: L25
• Publication date: 2016-10-12
• Acceptance date: 2016-09-16
• DOI: 10.3847/2041-8205/830/2/L25
• EISSN: 2041-8213
• ISSN: 2041-8205
• Keywords: turbulence; magnetic fields; waves; plasmas; galaxies: clusters: intracluster medium