Magnetar Activity via the Density-Shear Instability in Hall-MHD

TL;DR

This paper uses numerical simulations to demonstrate that the density-shear instability in Hall-MHD can create localized, intense magnetic structures in magnetar crusts, potentially powering magnetar activity and bursts.

Contribution

It provides the first non-linear simulation evidence that the density-shear instability can form strong, localized magnetic fields in magnetar crusts, influencing their activity.

Findings

The instability develops in various density and magnetic field profiles.

Localized magnetic structures with fields up to 10^15 G can form.

These structures can contain enough energy to power magnetar bursts.

Abstract

We investigate the density-shear instability in Hall-MHD via numerical simulation of the full non-linear problem, in the context of magnetar activity. We confirm the development of the instability of a plane-parallel magnetic field with an appropriate intensity and electron density profile, in accordance with analytic theory. We find that the instability also appears for a monotonically decreasing electron number density and magnetic field, a plane-parallel analogue of an azimuthal or meridional magnetic field in the crust of a magnetar. The growth rate of the instability depends on the Hall properties of the field (magnetic field intensity, electron number density and the corresponding scale-heights), while being insensitive to weak resistivity. Since the Hall effect is the driving process for the evolution of the crustal magnetic field of magnetars, we argue that this instability is critical for systems containing strong meridional or azimuthal fields. We find that this process mediates the formation of localised structures with much stronger magnetic field than the average, which can lead to magnetar activity and accelerate the dissipation of the field and consequently the production of Ohmic heating. Assuming a $5\times10^{14}$G magnetic field at the base of crust, we anticipate that magnetic field as strong as $10^{15}$G will easily develop in regions of typical size of a few $10^{2}$ meters, containing magnetic energy of $10^{43}$erg, sufficient to power magnetar bursts. These active regions are more likely to appear in the magnetic equator where the tangential magnetic field is stronger.