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arXiv 1204.0941astro-ph.HEastro-ph.CO
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GRB 080503中晚期再亮的成因

The origin of the late rebrightening in GRB 080503

R. Hascoët, F. Daigne, R. Mochkovitch

摘要:

雨燕探测到的GRB 080503属于爆发类,其瞬发相由一个初始的短尖峰和一个较长的软尾组成。它没有表现出任何过渡到一个定期余辉结束时的提示发射,但表现出一个令人惊讶的rebrightening后一天。我们的目标是解释这两种不同的情况下,刷新冲击或在环爆介质中的密度块的再亮和两个模型的余辉的起源,标准的一个,它来自前向冲击,和一个替代的一个,它的结果从一个长期的反向冲击。我们计算余辉光曲线,无论是使用单区近似的冲击区或详细的多区方法,更准确地占材料的压缩。我们发现,在几个考虑的情况下,必须使用详细的模型,以获得一个可靠的描述的冲击动力学。密度丛的情况是不赞成的。我们确认以前的结果,团块的存在下,向前冲击发射的影响不大,除非当冲击进入团块的微物理参数演变。此外,我们还发现用多区法计算逆激波的再亮也太弱。另一方面,在再流激波的情况下,在喷出物中的洛伦兹因子的分布和相对论流出的光束角的一些附加条件下,前向和反向激波模型都提供了令人满意的数据拟合。

英文摘要:

GRB 080503, detected by Swift, belongs to the class of bursts whose prompt phase consists of an initial short spike followed by a longer soft tail. It did not show any transition to a regular afterglow at the end of the prompt emission but exhibited a surprising rebrightening after one day. We aim to explain this rebrightening with two different scenarios - refreshed shocks or a density clump in the circumburst medium - and two models for the origin of the afterglow, the standard one where it comes from the forward shock, and an alternative one where it results from a long-lived reverse shock. We computed afterglow light curves either using a single-zone approximation for the shocked region or a detailed multizone method that more accurately accounts for the compression of the material. We find that in several of the considered cases the detailed model must be used to obtain a reliable description of the shock dynamics. The density clump scenario is not favored. We confirm previous results that the presence of the clump has little effect on the forward shock emission, except if the microphysics parameters evolve when the shock enters the clump. Moreover, we find that the rebrightening from the reverse shock is also too weak when it is calculated with the multi-zone method. On the other hand, in the refreshed-shock scenario both the forward and reverse shock models provide satisfactory fits of the data under some additional conditions on the distribution of the Lorentz factor in the ejecta and the beaming angle of the relativistic outflow.

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