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Special issue: Plasma physics of gamma-ray emission from the pulsars and their nebulae

Published online by Cambridge University Press:  03 May 2016

Jonathan Arons
Affiliation:
University of California, Astronomy, 501 Campbell Hall, Berkeley, CA 94720-3411, USA
Dmitri A. Uzdensky
Affiliation:
University of Colorado, CIPS, UCB 390, BOULDER, CO 80309-0390, USA
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Abstract

Information

Type
Editorial
Copyright
© Cambridge University Press 2016 
Figure 0

Figure 1. The Crab Nebula in 1–10 keV X-rays and optical light, from the Chandra and Hubble space observatories. The X-ray and optical torus extends approximately 1.8 light years in each direction, including the ‘jet’ structure. The image contracts with increasing photon energy, an effect of the loss of particle energy to synchrotron photon emission as the particles flow out from the central pulsar. The particles themselves are thought to be electrons and positrons created by conversion of gamma rays within the magnetosphere into $e^{\pm }$ pairs, while most of their energy is thought to come from shock wave acceleration and possibly magnetic reconnection occurring at the inner ring structure around the pulsar.

Figure 1

Figure 2. 0.1–10 GeV spectra of the Crab Nebula showing a prominent, day-long flare episode observed by the Fermi gamma-ray observatory in April, 2011. The dot-dash curve at the lower left is the quiescent synchrotron gamma-ray spectrum, while the lower solid curve is the total quiescent gamma-ray spectrum, including the Compton upscattered photons whose spectrum extends to 100 TeV. The gamma-ray telescopes have insufficient angular resolution to image the gamma-ray source, thus the exact location of the gamma-ray emission within the Nebula is unknown, although plausibly suspected to be from the inner part of the X-ray emitting region shown in figure 1.

Figure 2

Figure 3. Light curve of the Vela Pulsar. The observed photon fluxes, in 6 gamma-ray bands, plus X-rays, radio waves and ultraviolet waves, are plotted as a function of stellar rotation phase, where 0 to 1 represents stellar rotation from 0 to $2{\rm\pi}$ radians.