Constraining the Structure of GRB Jets Through the log(N)-log(S) Distribution
arXiv:astro-ph/0407063 · doi:10.1086/426664
Abstract
A general formalism is developed for calculating the luminosity function and the expected number of observed GRBs above a peak photon flux for any GRB jet structure. This new formalism directly provides the true GRB rate without the need for a `correction factor'. We apply it to the uniform jet (UJ) and universal structured jet (USJ) models for the structure of GRB jets and perform fits to the observed log(N)-log(S) distribution from the GUSBAD catalog which contains 2204 BATSE bursts. A core angle and an outer edge at are introduced for the structured jet, and a finite range of half-opening angles is assumed for the uniform jets. The efficiency for producing gamma-rays, and the energy per solid angle in the jet are allowed to vary with (the viewing angle ) in the UJ (USJ) model, and . We find that a single power-law luminosity function provides a good fit to the data. Such a luminosity function arises naturally in the USJ model, while in the UJ model it implies a power-law probability distribution for , . The value of cannot be directly determined from the fit to the observed log(N)-log(S) distribution, and an additional assumption on the value of or is required. Alternatively, an independent estimate of the true GRB rate would enable one to determine , and . The implied values of (or ) and are close to the current observational limits. The true GRB rate for the USJ model is found to be .
arXiv comment9 pages, 5 figures, 1 table; accepted for publication in ApJ
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