Abstract

Pulsars have been identified as good candidates for the acceleration of cosmic rays, up to ultra-high energies. However, a precise description of the acceleration processes at play is still to be established. Using 2D particle-in-cell simulations, we study proton acceleration in axisymmetric pulsar magnetospheres. Protons and electrons are extracted from the neutron star surface by the strong electric field induced by the rotation of the star, and electrons and positrons are produced in the magnetosphere through pair production process. As pair production has a crucial impact on electromagnetic fields, on gaps and thus on particle acceleration, we study its influence on the maximum energy and luminosity of protons escaping the magnetosphere. Protons are accelerated and escape in all our simulations. However, the acceleration sites are different for the protons and the pairs. As shown in previous studies, pairs are accelerated to their highest energies at the Y-point and in the equatorial current sheet, where magnetic reconnection plays an important role. In contrast, protons gain most of their kinetic energy below the light-cylinder radius within the separatrix current layers, but they are not confined within the equatorial current sheet. Their maximum Lorentz factors can reach 15% to 75% of the maximum Lorentz factor obtained by acceleration through the full vacuum potential drop from pole to equator, and increase with decreasing pair production. Their luminosity can reach 0.2% to 4% of the theoretical spin down luminosity of an aligned pulsar, and the minimum luminosity is obtained at the transition between the force-free and electrosphere regimes. These estimates support that millisecond pulsars could accelerate cosmic rays up to PeV energies and that new born millisecond pulsars could accelerate cosmic rays up to ultra-high energies.

Highlights

  • Pulsars are rapidly rotating and highly magnetized neutron stars, that have been detected across the entire electromagnetic spectrum, from radio to gamma rays

  • We focus on the two following fundamental questions: (i) what is the maximum energy achievable for the ions, especially for the ones escaping the magnetosphere, and (ii) to what level can they contribute to the observed high- and ultra-high-energy cosmic-ray fluxes? To this end, we perform particle-in-cell (PIC) simulations of the aligned pulsar magnetosphere

  • We use 2D PIC simulations to study the impact of pair production on the acceleration of protons in aligned pulsar magnetospheres

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Summary

Introduction

Pulsars are rapidly rotating and highly magnetized neutron stars, that have been detected across the entire electromagnetic spectrum, from radio to gamma rays (see e.g. Abdo et al 2013 for a Fermi-LAT catalog of gamma-ray pulsars and Aliu et al 2008; VERITAS Collaboration 2011; Aleksicet al. 2012 for the detection of the Crab pulsar above 100 GeV). Daugherty & Harding 1982; Gurevich & Istomin 1985; Zhang & Harding 2000; Medin & Lai 2010; Timokhin 2010; Timokhin & Arons 2013) are processes that remain to be fully understood and self-consistently implemented into large-scale systems This could have a critical influence on our understanding of pair multiplicities and highenergy emissions of pulsars, and might help to improve the models for energy dissipation and spin down. Chen & Beloborodov (2014) study an axisymmetric pulsar magnetosphere, where ions and electrons are injected from the neutron star surface and pairs can be produced. These latter authors notice the different trajectories of pairs and ions as well as the acceleration and escape of ions in different configurations.

Simulating a pulsar magnetosphere
Electromagnetic fields
Energy losses by radiation
Pair production
Simulation features
Plasma density
Pair multiplicity at the pole and Y-point
Charge and current densities
Particle acceleration and energy dissipation
Particle spectra
Trajectories and acceleration
Proton maximum energy in real pulsars
Energy dissipation and luminosity
Findings
Discussion and conclusions

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