Very high energy emission as a probe of relativistic magnetic reconnection in pulsar winds

TL;DR

This paper proposes that gamma-ray emissions from pulsars like Crab and Vela can be explained by synchrotron radiation from their striped wind current sheets, providing insights into relativistic magnetic reconnection physics.

Contribution

It introduces a model linking pulsar gamma-ray spectra to magnetic reconnection in striped winds, explaining spectral differences and predicting new observational signatures.

Findings

Crab and Vela gamma-ray spectra explained by synchrotron radiation from striped wind current sheets.

A new synchrotron self-Compton component is predicted for Crab by upcoming CTA observations.

Reconnection regimes differ between energetic and less energetic pulsars, affecting particle spectra.

Abstract

The population of gamma-ray pulsars, including Crab observed in the TeV range, and Vela detected above 50 GeV, challenges existing models of pulsed high-energy emission. Such models should be universally applicable, yet they should account for spectral differences among the pulsars. We show that the gamma-ray emission of Crab and Vela can be explained by synchrotron radiation from the current sheet of a striped wind, expanding with a modest Lorentz factor $\Gamma\lesssim100$ in the Crab case, and $\Gamma\lesssim50$ in the Vela case. In the Crab spectrum a new synchrotron self-Compton component is expected to be detected by the upcoming experiment CTA. We suggest that the gamma-ray spectrum directly probes the physics of relativistic magnetic reconnection in the striped wind. In the most energetic pulsars, like Crab, with $\dot{E}_{38}^{3/2}/P_{-2}\gtrsim0.002$ (where $\dot{E}$ is the spin down power, $P$ is the pulsar period, and $X=X_i\times10^i$ in CGS units), reconnection proceeds in the radiative cooling regime and results in a soft power-law distribution of cooling particles; in less powerful pulsars, like Vela, particle energization is limited by the current sheet size, and a hard particle spectrum reflects the acceleration mechanism. A strict lower limit on the number density of radiating particles corresponds to emission close to the light cylinder, and, in units of the GJ density, it is $\gtrsim0.5$ in the Crab wind, and $\gtrsim0.05$ in the Vela wind.