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arXiv 1503.07513astro-ph.HE
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伽马射线暴121024 A的微观物理和动力学

Microphysics and dynamics of the Gamma-Ray Burst 121024A

K. Varela, H. van Eerten, J. Greiner, P. Schady, J. Elliott, V. Sudilovsky, T. Krühler, A. J. van der Horst, J. Bolmer, F. Knust, C. Agurto, F. Azagra, A. Bello… 展开作者

K. Varela, H. van Eerten, J. Greiner, P. Schady, J. Elliott, V. Sudilovsky, T. Krühler, A. J. van der Horst, J. Bolmer, F. Knust, C. Agurto, F. Azagra, A. Belloche, F. Bertoldi, C. De Breuck, C. Delvaux, R. Filgas, J. Graham, A. Nicuesa Guelbenzu, D. A. Kann, S. Klose, K. M. Menten, A. Rau, A. Rossi, S. Schmidl, F. Schuller, T. Schweyer, M . Tanga, A. Weiss, P. Wiseman, F. Wyrowski

摘要:

目标。该研究的目的是通过分析GRB 121024 A的多波长余辉数据集来限制伽马射线暴(GRB)的物理学,该数据集涵盖了从无线电到X射线的全部范围。方法.利用GRB 121024 A余辉的多历元宽带观测,我们测量了同步辐射谱的三个特征突变频率。我们使用了六个时期的组合XRT和GROND数据来约束时间斜率,尘埃消光,X射线吸收和光谱斜率具有高精度。来自XRT、GROND、APEX、CARMA和EVLA的组合数据的另外两个时期用于对断裂频率以及因此对微物理和动力学参数设置约束。结果XRT和GROND光变曲线显示在49 k左右同时发生消色差的突变。因此,同步加速器冷却中断的交叉不能适当解释光变曲线的中断。多波长数据使我们能够测试两种解释断裂的可能性:射流断裂和能量注入结束。喷流中断方案需要一个硬的电子谱,一个非常低的冷却中断频率,和一个非扩散喷流。能量注入避免了这些问题,但需要$ε_e > 1 (k = 2)$、球形流出和$ε_B < 10^{-9}$。结论.鉴于能量注入模型所需的极端微物理参数,我们倾向于使用$ν_m < ν_{sa}$来解释观测结果的射流破碎情景。这种情况下给出了物理上有意义的微物理参数,它也自然地解释了线性和圆偏振的检测报告。

英文摘要:

Aims. The aim of the study is to constrain the physics of gamma-ray bursts (GRBs) by analysing the multi-wavelength afterglow data set of GRB 121024A that covers the full range from radio to X-rays. Methods. Using multi-epoch broad-band observations of the GRB 121024A afterglow, we measured the three characteristic break frequencies of the synchrotron spectrum. We used six epochs of combined XRT and GROND data to constrain the temporal slopes, the dust extinction, the X-ray absorption, and the spectral slope with high accuracy. Two more epochs of combined data from XRT, GROND, APEX, CARMA, and EVLA were used to set constraints on the break frequencies and therefore on the micro-physical and dynamical parameters. Results. The XRT and GROND light curves show a simultaneous and achromatic break at around 49 ks. As a result, the crossing of the synchrotron cooling break is no suitable explanation for the break in the light curve. The multi wavelength data allow us to test two plausible scenarios explaining the break: a jet break, and the end of energy injection. The jet-break scenario requires a hard electron spectrum, a very low cooling break frequency, and a non-spreading jet. The energy injection avoids these problems, but requires $ε_e > 1 (k = 2)$, spherical outflow, and $ε_B < 10^{-9}$. Conclusions. In light of the extreme microphysical parameters required by the energy-injection model, we favour a jet-break scenario where $ν_m < ν_{sa}$ to explain the observations. This scenario gives physically meaningful microphysical parameters, and it also naturally explains the reported detection of linear and circular polarisation.

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