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On the Origin and Evolution of Curvature of the Spectral Energy Distribution of Fermi Bright Blazars

机译:论FERMI BIGHT BLAZARS光谱能量分布曲率的起源与演变

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The origin and evolution of spectral curvature in blazar spectral energy distribution (SED) is still unclear. Since the observed SED curvature is related to an intrinsic curvature in emitting electron energy distribution (EED), we study this question by employing a log-parabolic EED with a curvature parameter and peak energy to model the quasi-simultaneous broadband SEDs of selected blazars in the Fermi-LAT Bright AGN Sample using synchrotron and inverse Compton (IC) processes. We find that the log-parabolic IC model can successfully explain the emission in all blazars in our sample. On average, FSRQs have higher magnetic field, Doppler factor, and curvature than BL Lac objects. The BL Lac objects show an anticorrelation between the curvature parameter of the EED and its peak energy, which is a signature of stochastic acceleration. FSRQs do not manifest such correlation and rather show a mild positive relationship between these parameters. This suggests that the evolution of spectral curvature in the BL Lac objects is dominated by a strong stochastic acceleration component, whereas the curvature in FSRQs evolves in a cooling dominated regime due to an additional external Compton component. The strong cooling in FSRQs not only restricts the electron peak energy but also adds extra curvature to the high energy tail of emitting EED. Since the curvature decreases from FSRQs toward high peak BL Lac objects (HBLs), opposite to peak energy, the curvature parameter can be considered a third parameter of the blazar sequence in addition to peak frequency and luminosity.
机译:波拉格光谱能量分布(SED)中光谱曲率的起源和演变仍不清楚。由于观察到的SED曲率与发射电子能量分布(EED)中的内在曲率有关,因此我们通过使用曲率参数和峰值能量的Log-抛物线来研究该问题,以模拟所选布拉恩的准同声宽带SED。 Fermi-Lat Bright Agn使用SynchRotron和Inverse Compton(IC)过程的样品。我们发现,Log-Parabolic IC模型可以成功解释我们样本中所有布拉齐的排放。平均而言,FSRQ具有更高的磁场,多普勒因子和曲率,而不是BL LAC对象。 BL LAN对象在EED的曲率参数及其峰值能量之间显示出逆相关,这是随机加速的签名。 FSRQ不表现出这样的相关性,而是在这些参数之间表现出温和的正相关关系。这表明BL LAC对象中光谱曲率的演变由强大的随机加速度组成,而FSRQ中的曲率由于另外的外部康普顿组分而在冷却主导的状态下演变。 FSRQ中的强化冷却不仅限制了电子峰值能量,而且还为发射eed的高能量尾添加了额外的曲率。由于曲率从FSRQ朝向高峰值BL LAC对象(HBL)的曲率减小,因此除了峰值频率和发光度之外,曲率参数还可以被认为是Blazar序列的第三参数。

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