Radio polarimetry signatures of strong magnetic turbulence in Supernova Remnants

TL;DR

This paper models how strong magnetic turbulence affects polarized radio emissions from supernova remnants, revealing how turbulence anisotropy and internal Faraday rotation influence polarization signatures.

Contribution

It introduces a model linking magnetic turbulence characteristics to radio polarization signatures in supernova remnants, incorporating anisotropy and Faraday rotation effects.

Findings

Isotropic turbulence yields weak polarization without Faraday rotation.

Anisotropic turbulence can significantly increase polarization degree.

Model matches Tycho's remnant data, constraining turbulence amplitude.

Abstract

We discuss the emission and transport of polarized radio-band synchrotron radiation near the forward shocks of young shell-type supernova remnants, for which X-ray data indicate a strong amplification of turbulent magnetic field. Modeling the magnetic turbulence through the superposition of waves, we calculate the degree of polarization and the magnetic polarization direction which is at $90^\circ$ to the conventional electric polarization direction. We find that isotropic strong turbulence will produce weakly polarized radio emission even in the absence of internal Faraday rotation. If anisotropy is imposed on the magnetic-field structure, the degree of polarization can be significantly increased, provided internal Faraday rotation is inefficient. Both for shock compression and a mixture with a homogeneous field, the increase in polarization degree goes along with a fairly precise alignment of the magnetic-polarization angle with the direction of the dominant magnetic-field component, implying tangential magnetic polarization at the rims in the case of shock compression. We compare our model with high-resolution radio polarimetry data of Tycho's remnant. Using the absence of internal Faraday rotation we find a soft limit for the amplitude of magnetic turbulence, $\delta B \lesssim 200\ {\rm \mu G}$. The data are compatible with a turbulent magnetic field superimposed on a radial large-scale field of similar amplitude, $\delta B\simeq B_0$. An alternative viable scenario involves anisotropic turbulence with stronger amplitudes in the radial direction, as was observed in recent MHD simulations of shocks propagating through a medium with significant density fluctuations.