论文标题

基于光谱能量分布的分析,Blazar MRK 421的物理参数的变化

Variations of the physical parameters of the blazar Mrk 421 based on the analysis of the spectral energy distributions

论文作者

Yamada, Yurika, Uemura, Makoto, Itoh, Ryosuke, Fukazawa, Yasushi, Ohno, Masanori, Imazato, Fumiya

论文摘要

我们报告了在Blazar MRK 421中观察到的射流物理参数的变化,并根据对几种光谱能分布(SEDS)的分析,讨论射流中X射线耀斑的起源。 SED是使用单区同步加速器自compton(SSC)模型及其参数使用Markov Chain Monte Carlo方法确定的。 TEV能量缺乏数据意味着许多参数不能唯一确定并相关。这些是详细研究的。我们发现,只有当我们将约束应用于四个参数之一时,才能唯一确定最佳解决方案:磁场(b),多普勒因子,发射区域的大小和电子能量分布的归一化因子。从2009年到2014年,我们使用了31组SED,并使用UVOT/SWIFT和KANATA望远镜观察到光学 - UV数据,带有XRT/Swift的X射线数据以及带有费米大面积望远镜(LAT)的伽马射线数据。我们的SED分析结果表明,在X射线微弱状态下,发射发生在相对较小的面积(〜10^16 cm)中,具有相对较强的磁场(B〜10^-1 g)。 X射线明亮的状态显示出与微弱状态相反的趋势,即较大的发射区域(〜10^18厘米),可能在射流和弱磁场的下游(B〜10^-3 g)。高X射线通量是由于电子的最大能量增加。另一方面,存在两种发射区域的存在意味着单区模型不适合繁殖,至少一部分观察到的SED。

We report on the variations of the physical parameters of the jet observed in the blazar Mrk 421, and discuss the origin of X-ray flares in the jet, based on the analysis of the several spectral energy distributions (SEDs). The SEDs are modeled using the one-zone synchrotron self-Compton (SSC) model and its parameters determined using a Markov chain Monte Carlo method. The lack of data at TeV energies means many of the parameters cannot be uniquely determined and are correlated. These are studied in detail. We found that the optimal solution can be uniquely determined only when we apply a constraint to one of four parameters: the magnetic field (B), Doppler factor, size of the emitting region, and normalization factor of the electron energy distribution. We used 31 sets of SED from 2009 to 2014 with optical-UV data observed with UVOT/Swift and the Kanata telescope, X-ray data with XRT/Swift, and gamma-ray data with the Fermi Large Area Telescope (LAT). The result of our SED analysis suggests that, in the X-ray faint state, the emission occurs in a relatively small area (~ 10^16 cm) with relatively strong magnetic field (B~10^-1 G). The X-ray bright state shows a tendency opposite to that of the faint state, that is, a large emitting area (~10^18 cm), probably in the downstream of the jet and weak magnetic field (B~10^-3 G). The high X-ray flux was due to an increase in the maximum energy of electrons. On the other hand, the presence of two kinds of emitting areas implies that the one-zone model is unsuitable to reproduce, at least a part of the observed SEDs.

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