General-relativistic force-free pulsar magnetospheres

TL;DR

This paper models general-relativistic effects on pulsar magnetospheres using simulations, revealing how gravity and frame-dragging influence electromagnetic emissions and pulsar luminosity.

Contribution

It provides the first detailed time-dependent simulations of relativistic pulsar magnetospheres with realistic magnetic configurations, incorporating gravitational effects.

Findings

Relativistic effects can increase Poynting flux by up to a factor of 2.

Luminosity follows a sin^2(chi) dependence on obliquity.

Angular distribution of flux varies with pulsar orientation, scaling as sin^2(theta) or sin^4(theta).

Abstract

Pulsar magnetospheres are shaped by ultra-relativistic electron/positron plasmas flowing in a strong magnetic field and subject to strong gravitational fields. The former induces magnetospheric currents and space charges responsible for the distortion of the electromagnetic field based on pure electrodynamics. The latter induces other perturbations in these fields based on space-time curvature. The force-free approximation describes the response of this magnetosphere to the presence of currents and charges and has been investigated by many authors. In this context, general relativity has been less discussed to quantify its influence on the neutron star electrodynamics. It is the purpose of this paper to compute general-relativistic force-free pulsar magnetospheres for realistic magnetic field configurations such as the inclined dipole. We performed time-dependent simulations of Maxwell equations in the 3+1 formalism of a stationary background metric in the slow-rotation approximation. We computed the resulting Poynting flux depending on the ratio~$R/\rlight$ and on frame-dragging through the spin parameter~$\as$, $R$ is the neutron star radius and $\rlight$ the light-cylinder radius. Both effects act together to increase the total Poynting flux seen by a distant observer by a factor up to~2 depending on the rotation rate. Moreover we retrieve the $\sin^2\chi$ dependence of this luminosity, $\chi$ being the obliquity of the pulsar, as well as a braking index close to $n=3$. We also show that the angular dependence of the Poynting flux scales like $\sin^2\vartheta$ for the aligned rotator but like $\sin^4\vartheta$ for the orthogonal rotator, $\vartheta$ being the colatitude.