Abstract
Abstract The curvature effect may be responsible for the steep decay phase observed in gamma-ray bursts. To test the curvature effect with observations, the zero time point t 0 adopted to plot the observer time and flux on a logarithmic scale should be appropriately selected. In practice, however, the true t 0 cannot be directly constrained from the data. Thus, we move t 0 to a certain time in the steep decay phase, which can be easily identified. In this situation, we derive an analytical formula to describe the flux evolution of the steep decay phase. The analytical formula reads as with , where F ν is the flux observed at frequency ν, is the observer time by setting t 0 at a certain time in the steep decay phase, β is the spectral index estimated around ν, and is the decay timescale of the phase with . We test the analytical formula with the data from numerical calculations. It is found that the analytical formula presents a good estimate of the evolution of the flux shaped by the curvature effect. Our analytical formula can be used to confront the curvature effect with observations and estimate the decay timescale of the steep decay phase.
Highlights
Gamma-ray bursts (GRBs) are the most powerful explosive events in the Universe
Fν is the flux observed at frequency ν, tobs is the observer time by setting zero time point t0 at a certain time in the steep decay phase, β is the spectral index estimated around ν, and tc is the decay timescale of the phase with tobs 0
It is found that the analytical formula presents a well estimation about the evolution of flux shaped by the curvature effect
Summary
Gamma-ray bursts (GRBs) are the most powerful explosive events in the Universe. They are always traced by the Burst Alert Telescope (BAT) in the γ-ray energy bands (Barthelmy et al 2005a). If one wants to find the relation as Equation (1) based on the observational data, the time t0 for the steep decay phase should be appropriately selected. This is because the light curves of GRB are plotted on a logarithmic scale for both the observer time and the flux in order to find the decay slope α. One practical way to test the curvature effect model may be to move t0 to a certain time in the steep decay phase, which can be identified in the GRB light curves. By moving t0 to a certain time in the steep decay phase, the analytical formula of flux evolution is presented and tested in Sections 3 and 4, respectively.
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