Abstract

Context. The formation of a large-scale current sheet is a generic feature of pulsar magnetospheres. If the magnetic axis is misaligned with the star rotation axis, the current sheet is an oscillatory structure filling an equatorial wedge determined by the inclination angle, known as the striped wind. Relativistic reconnection could lead to significant dissipation of magnetic energy and particle acceleration, although the efficiency of this process is debated in this context. Aims. In this study, we aim at reconciling global models of pulsar wind dynamics and reconnection in the stripes within the same numerical framework in order to shed new light on dissipation and particle acceleration in pulsar winds. Methods. To this end, we perform large three-dimensional particle-in-cell simulations of a split-monopole magnetosphere, from the stellar surface up to 50 light-cylinder radii away from the pulsar. Results. Plasmoid-dominated reconnection efficiently fragments the current sheet into a dynamical network of interacting flux ropes separated by secondary current sheets that consume the field efficiently at all radii, even past the fast magnetosonic point. Our results suggest there is a universal dissipation radius solely determined by the reconnection rate in the sheet, lying well upstream from the termination shock radius in isolated pair-producing pulsars. The wind bulk Lorentz factor is much less relativistic than previously thought. In the co-moving frame, the wind is composed of hot pairs trapped within flux ropes with a hard broad power-law spectrum, whose maximum energy is limited by the magnetization of the wind at launch. Conclusions. We conclude that the striped wind is most likely fully dissipated when it enters the pulsar wind nebula. The predicted wind particle spectrum after dissipation is reminiscent of the Crab Nebula radio-emitting electrons.

Highlights

  • Large-scale current sheets are generic features of planetary and stellar magnetospheres

  • We propose a simple analytical model for the evolution of magnetic dissipation inspired by our simulations in an attempt to extrapolate our results to realistic pulsar winds

  • We find that the upstream magnetic field strength at the trailing edge of the sheet, Buφp, is on the order of the ideal split monopole field at all radii, even though the striped-averaged field strength decreases with radius due to dissipation, that is: Buφp such that the sheet is always fed with a fresh, non-reconnected magnetic field

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Summary

Introduction

Large-scale current sheets are generic features of planetary and stellar magnetospheres Their formation can be externally driven, as in the Earth magnetotail shaped by the Solar wind, or internally driven by the intrinsic magnetic activity of the star or by the rapid rotation of the magnetosphere, like in Jupiter. The magnetic and current structures are supported by a plasma of relativistic electron-positron pairs that are self-generated near the stellar surface via pair production. This plasma flows along open field lines in the form of a radially expanding, relativistic magnetized wind, referred to as the pulsar wind in the following (Rees & Gunn 1974; Kennel & Coroniti 1984)

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