4.7 Article

The importance of off-jet relativistic kinematics in gamma-ray burst jet models

Journal

ASTROPHYSICAL JOURNAL
Volume 645, Issue 1, Pages 436-449

Publisher

IOP PUBLISHING LTD
DOI: 10.1086/504255

Keywords

gamma rays : bursts; ISM : jets and outflows; shock waves

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GRBs are widely thought to originate from collimated jets of material moving at relativistic velocities. Emission from such a jet should be visible even when viewed from outside the angle of collimation. I summarize recent work on the special relativistic transformation of the burst quantities E-iso (isotropic-equivalent energy of the burst) and E-peak (peak of the burst spectrum in the power nu F-nu) as a function of viewing angle. The resulting formulae serve as input for a Monte Carlo population synthesis method, with which I investigate the importance of off-jet relativistic kinematics as an explanation for a class of GRBs termed X-ray flashes (XRFs) in the context of several top-hat-shaped variable opening-angle jet models. For certain parameters, such models predict a large population of off-jet bursts that are observable and that lie away from the E-peak proportional to E-iso(1/2) relation. This predicted burst population is not seen in current data sets. I investigate the effect of the bulk gamma value on the properties of this population of off-jet bursts, as well as the effect of including an Omega(0)-E-gamma correlation to jointly fit the E-peak proportional to E-iso(1/2) and E-peak proportional to E-gamma(beta) relations, where Omega(0) is the opening solid angle of the GRB jet. I find that the XRFs seen by HETE-2 and BeppoSAX cannot be easily explained as classical GRBs viewed off-jet. I also find that an inverse correlation between gamma and Omega(0) has the effect of greatly reducing the visibility of off-jet events. Therefore, unless gamma > 300 for all bursts, or there is a strong inverse correlation between gamma and Omega(0), top-hat variable opening-angle jet models produce a significant population of bursts away from the E-peak proportional to E-iso(1/2) and E-peak proportional to E-gamma(beta) relations, in contradiction with current observations.

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