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CONSTRAINING GAMMA-RAY BURST INITIAL LORENTZ FACTOR WITH THE AFTERGLOW ONSET FEATURE AND DISCOVERY OF A TIGHT Γ<sub>0</sub>-<i>E</i><sub>γ,iso</sub>CORRELATION

En‐Wei LiangDepartment of Physics and Astronomy, University of Nevada, Las Vegas, NV 89154, USA; [email protected]Shuang-Xi YiDepartment of Physics, Guangxi University, Nanning 530004, China; [email protected]Jin ZhangCollege of Physics and Electronic Engineering, Guangxi Teachers Education University, Nanning, Guangxi 530001, ChinaHou-Jun LüDepartment of Physics, Guangxi University, Nanning 530004, China; [email protected]Bin‐Bin ZhangDepartment of Physics and Astronomy, University of Nevada, Las Vegas, NV 89154, USA; [email protected]Bing ZhangDepartment of Physics and Astronomy, University of Nevada, Las Vegas, NV 89154, USA; [email protected]
2010en
ABI

Аннотация

The onset of GRB afterglow is characterized by a smooth bump in the early afterglow lightcurve. We make an extensive search for such a feature. Twenty optically selected GRBs and 12 X-ray selected GRBs are found, among which 17 optically selected GRBs and 2 X-ray-selected GRBs have redshift measurements. We fit the lightcurves with a smooth broken power-law and measure the temporal characteristic timescales of the bumps at FWHM. Strong mutual correlations among these timescales are found, and a dimmer and broader bump tends to peak at a later peak time. The ratio of rising to decaying timescales is almost universal among bursts, but the ratio of the rising time to the peak time varies from 0.3~1. The E_iso is tightly correlated with the peak luminosity and the peak time of the bump in the burst frame. Assuming that the bumps signal the deceleration of the GRB fireballs in a constant density medium, we calculate the initial Lorentz factor (Gamma_0) and the deceleration radius (R_dec) of the GRBs in the optical-selected sample. It is found that Gamma_0 are typically a few hundreds, and the typical deceleration radius is R_dec~10^{17} cm. More intriguingly, a tight correlation between the Gamma_0 and E_iso is found, namely Gamma_0 ~ 195 E_iso, 52}^{0.27} (satisfied for both the optical and X-ray z-known samples). It is helpful to understand GRB physics, and may serve as an indicator of Gamma_0. We find that the early bright X-rays are usually dominated by a different component from the external shock emission, but occasionally (for one case) an achromatic deceleration feature is observed. Components in X-rays would contribute to the diversity of the observed X-ray lightcurves (abridge).

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