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A Statistical Comparison of the Optical/UV and X-ray Afterglows of Gamma-Ray Bursts using the Swift Ultra-violet Optical and X-ray Telescopes

机译:光学/紫外和X射线余辉的统计比较   伽玛射线爆发使用swift紫外光学和X射线望远镜

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摘要

We present the systematic analysis of the UVOT and XRT light curves for asample of 26 Swift Gamma-Ray Bursts (GRBs). By comparing the optical/UV andX-ray light curves, we found that they are remarkably different during thefirst 500s after the BAT trigger, while they become more similar during themiddle phase of the afterglow, i.e. between 2000s and 20000s. If we takeliterally the average properties of the sample, we find that the mean temporalindices observed in the optical/UV and X-rays after 500s are consistent with aforward-shock scenario, under the assumptions that electrons are in the slowcooling regime, the external medium is of constant density and the synchrotroncooling frequency is situated between the optical/UV and X-ray observing bands.While this scenario describes well the averaged observed properties, someindividual GRB afterglows require different or additional assumptions, such asthe presence of late energy injection. We show that a chromatic break (a breakin the X-ray light curve that is not seen in the optical) is present in theafterglows of 3 GRBs and demonstrate evidence for chromatic breaks in a further4 GRBs. The average properties of these breaks cannot be explained in terms ofthe passage of the synchrotron cooling frequency through the observed bands,nor a simple change in the external density. It is difficult to reconcilechromatic breaks in terms of a single component outflow and instead, morecomplex jet structure or additional emission components are required.
机译:我们介绍了26个Swift伽马射线暴(GRB)样本的UVOT和XRT光曲线的系统分析。通过比较光学/ UV和X射线光曲线,我们发现它们在BAT触发后的前500 s期间有显着差异,而在余辉的中间阶段(即2000到20000 s之间)则变得更加相似。如果我们将样品的平均特性归类,我们发现在500s之后的光学/ UV和X射线中观察到的平均时间指标与前向冲击的情况是一致的,前提是电子处于慢冷状态,即外部介质尽管这种情况很好地描述了平均观察到的特性,但是某些GRB余辉需要不同或附加的假设,例如是否存在后期能量注入。我们显示在3个GRB的余辉中存在色差(在光学中看不到的X射线光曲线的断裂),并证明了另外4个GRB中色差的证据。这些断裂的平均特性不能用同步加速器冷却频率通过观察到的频带的方式来解释,也不能通过外部密度的简单变化来解释。就单组分流出而言,很难协调色差,相反,需要更复杂的射流结构或附加的发射组分。

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