An investigation of magnetic field distortions in accretion discs around neutron stars. I. Analysis of the poloidal field component

TL;DR

This study models stationary magnetic field configurations in accretion discs around magnetized neutron stars, analyzing how turbulence and flow affect the poloidal magnetic field structure through numerical solutions.

Contribution

It introduces a local magnetic distortion function to better understand magnetic field distortions in accretion discs, improving upon previous global parameter approaches.

Findings

Distortions increase with magnetic Reynolds number R_m.

Significant field weakening occurs where D_m>1.

Transition zones show amplified fields with variable minima and maxima.

Abstract

We report results from calculations investigating stationary magnetic field configurations in accretion discs around magnetised neutron stars. Our strategy is to start with a very simple model and then progressively improve it providing complementary insight into results obtained with large numerical simulations. In our first model, presented here, we work in the kinematic approximation and consider the stellar magnetic field as being a dipole aligned with the stellar rotation axis and perpendicular to the disc plane, while the flow in the disc is taken to be steady and axisymmetric. The behaviour in the radial direction is then independent of that in the azimuthal direction. We investigate the distortion of the field caused by interaction with the disc matter, solving the induction equation numerically in full 2D. The influence of turbulent diffusivity and fluid velocity on the poloidal field configuration is analysed, including discussion of outflows from the top and bottom of the disc. We find that the distortions increase with increasing magnetic Reynolds number R_m (calculated using the radial velocity). However, a single global parameter does not give an adequate description in different parts of the disc and we use instead a `magnetic distortion function' D_m(r,\theta) (a magnetic Reynolds number defined locally). Where D_m<<1 (near to the inner edge of the disc) there is little distortion, but where D_m>1 (most of the rest of the disc), there is considerable distortion and the field becomes weaker than the dipole would have been. Between these two regions, there is a transition zone where the field is amplified and can have a local minimum and maximum. The location of this zone depends sensitively on the diffusivity. The results depend very little on the boundary conditions at the top of the disc.