论文标题
Blazar喷气式喷气机以每个Baryon的能源相似,独立于他们的力量
Blazar jets launched with similar energy per baryon, independently of their power
论文作者
论文摘要
最极端活跃的银河系核(AGN)是无线电活动的相对论射流传播靠近我们的视线。这些对象首先根据其发射线特征分类为平面无线电类星体(FSRQ)和Bl lacertae对象(BL LACS)。最近,观察结果揭示了这些被称为\ emph {blazar序列}的对象之间的趋势,以及观察到的功率与同步峰的频率之间的抗相关性。在目前的工作中,我们提出了一个相当简单的想法,可以解释整个Blazar人口:所有喷气机的每台巴里昂都与他们的力量无关。在FSRQ的情况下,如无线电中观察到的那样,最强大的喷气机设法加速到较高的Lorentz因子。结果,它们在发射区域具有相当适度的磁化,从而导致磁重新连接注入陡峭的颗粒能分布,因此在$γ$ rays中陡峭的发射光谱。对于较弱的喷气机,即Bl lacs,相反的是真实的;即,射流没有达到非常高的洛伦兹因子,从而导致更多可用于非热粒子加速的磁能,而在频率上以$ \ gtrsim $ GEV处的更硬发射光谱。在这种情况下,我们使用模拟恢复了Blazars的所有可观察性能,包括\ emph {Blazar序列},用于轻度baryon载荷的模型($ 50 \ lyssim -simμ\ Lessim 80 $)。因此,这种对Blazar种群的解释严重限制了Blarazar喷气机的能量,无论其吸积率如何。
The most extreme active galactic nuclei (AGN) are the radio active ones whose relativistic jet propagates close to our line of sight. These objects were first classified according to their emission line features into flat-spectrum radio quasars (FSRQs) and BL Lacertae objects (BL Lacs). More recently, observations revealed a trend between these objects known as the \emph{blazar sequence}, along with an anti-correlation between the observed power and the frequency of the synchrotron peak. In the present work, we propose a fairly simple idea that could account for the whole blazar population: all jets are launched with similar energy per baryon, independently of their power. In the case of FSRQs, the most powerful jets, manage to accelerate to high bulk Lorentz factors, as observed in the radio. As a result, they have a rather modest magnetization in the emission region, resulting in magnetic reconnection injecting a steep particle energy distribution and, consequently, steep emission spectra in the $γ$-rays. For the weaker jets, namely BL Lacs, the opposite holds true; i.e., the jet does not achieve a very high bulk Lorentz factor, leading to more magnetic energy available for non-thermal particle acceleration, and harder emission spectra at frequencies $\gtrsim$ GeV. In this scenario, we recover all observable properties of blazars with our simulations, including the \emph{blazar sequence} for models with mild baryon loading ($50 \lesssim μ\lesssim 80$). This interpretation of the blazar population, therefore, tightly constrains the energy per baryon of blazar jets regardless of their accretion rate.