Abstract.
The main target of this study is the GRB light curve during the decay phase of long, bright pulses. As shown by Ryde & Svensson (2000; hereafter RS00) approximately half of these decays can be described by a power law \(\propto 1\)/(time). This happens for cases when the hardness-fluence correlation (HFC) is an exponential function, \(E_{\rm pk}(\Phi) \propto e^{-\Phi/\Phi_0}\), and the hardness-intensity correlation (HIC) is a power law, \(E_{\rm pk}(N) \propto (N/N_0)^{\delta}\). Here, N(t) is the instantaneous photon flux, \(E_{\rm pk}(t)\) is the corresponding photon energy, at which the \(E^2 N_{\rm E}\)-spectrum peaks and is used as a measure of the spectral hardness, and the photon fluence is defined by \(\Phi(t) = \int^t N(t') dt'\). These most commonly assumed correlations were found by Liang & Kargatis (1996; HFC) and Golenetskii et al. (1983; HIC).
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Ryde, F., Svensson, R. A Variety of Decays of Gamma-Ray Burst Pulses. In: Costa, E., Frontera, F., Hjorth, J. (eds) Gamma-Ray Bursts in the Afterglow Era. ESO ASTROPHYSICS SYMPOSIA. Springer, Berlin, Heidelberg. https://doi.org/10.1007/10853853_22
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DOI: https://doi.org/10.1007/10853853_22
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