Pulsar wind nebulae with bow shocks: non-thermal radiation and cosmic ray leptons

Abstract

Pulsars with high spin-down power produce relativistic winds radiating a fraction of the power in the range from radio to gamma-rays in the pulsar wind nebulae (PWNe). The rest of the power is dissipated in the interactions of the PWNe with the interstellar medium (ISM). Some of the PWNe are moving relative to the ISM with supersonic speeds producing bow shocks. In this case, the ultrarelativistic particles accelerated at the termination surface of the pulsar wind may be reaccelerated in the converging flow system formed by the outflow from the wind termination shock and the inflow from the bow shock. An outcome of this reacceleration is the creation of particle distributions with hard spectra, such as required to explain the observed synchrotron spectra with photon indices Gamma <~ 1.5. The presence of this hard component is specific to PWNe with bow shocks (BSPWNe). The accelerated particles may end up containing a substantial fraction of the shock ram pressure. For typical ISM and pulsar parameters, the positrons released by these systems are numerous enough to contribute a substantial fraction of the positrons detected as galactic cosmic ray particles above few tens and up to several hundred GeV. The escape of ultrarelativistic particles from a BSPWN and its appearance in the far-UV and X-ray bands is determined by the directions of the interstellar magnetic field, the velocity of the astrosphere and the pulsar rotation axis. In this respect we review the observed appearance and multiwavelength spectra of three different types of BSPWNe: PSR J0437-4715, the Guitar and Lighthouse nebulae, and Vela-like objects. We argue that high resolution imaging of such objects provides unique information on pulsar winds and on the ISM. We discuss the interpretation of imaging observations and estimate the BSPWN contribution to the positron flux observed at the Earth. (ABRIDGED)

69 pages, 18 figures, Space Science Reviews (in press) 2017

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