A STRINGENT LIMIT ON THE AMPLITUDE OF ALFVENIC PERTURBATIONS IN HIGH-BETA LOW-COLLISIONALITY PLASMAS

It is shown that low-collisionality plasmas cannot support linearly polarized shear-Alfven fluctuations above a critical amplitude delta B-perpendicular to/B-0 similar to beta(-1/2), where beta 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-Alfven-wave amplitudes has far-reaching implications for the physics of magnetized turbulence in the high-beta conditions prevalent in many astrophysical plasmas, as well as for the solar wind at similar to 1 au where beta greater than or similar to 1.