论文标题

在2010年和2014年的Blazar 3C 454.3的弹性特征行为差异和光谱特征行为的差异

Multiwavelength analysis and the difference in the behavior of the spectral features during the 2010 and 2014 flaring periods of the blazar 3C 454.3

论文作者

Amaya-Almazán, Raúl Antonio, Chavushyan, Vahram, Patiño-Álvarez, Victor Manuel

论文摘要

多年来,平面光谱无线电排3c〜454.3呈现出很高的活性阶段(耀斑),其中不同的波带大大增加了磁通量。在这项工作中,我们进行了从无线电到伽马射线的多波强长分析,并研究Mg〜II〜 $λ2798$Å发射线和2008-2018的UV〜FE〜II频段。我们发现,准平台分量C的43 GHz通量密度增加,与估计的时间相吻合,在该估计的时间中,从无线电核心弹出的超光孔(导致2010年最亮的火炬)与准平稳的组件相撞(在$ \ sim4.6 $ pc pc pc pc pc pc coldeptionary组件(预定的距离)。频谱索引在第一个($ 5000 <\ text {jd} -2450000 <5600 $)和第二个($ 6600 <\ text {jd} -2450000 <7900 $)燃烧时期表明,物理条件的变化。第二阶段的复杂性质可能是在不同位置叠加多个事件的结果。 Mg〜II与UV-Continuum具有抗相关性,而Fe〜II呈正相关。除了在2010年最亮的耀斑时期,当时两者在高连续体的光度下都有强烈的反应。我们的结果表明,第一个燃烧时期的主要伽马射线排放机制是康普顿外部。在第二张耀斑期间,种子光子发射区域与伽马射线发射区域是共同空间的。但是,需要使用多Zone射流发射模型进行SED研究,以确认第二阶段的每个有明显耀斑的性质。

The flat-spectrum radio quasar 3C~454.3 throughout the years has presented very high activity phases (flares) in which the different wavebands increase their flux dramatically. In this work, we perform multiwavelength analysis from radio to gamma-rays and study the Mg~II~$λ2798$Å emission line and the UV~Fe~II band from 2008-2018. We found that an increase in the 43 GHz flux density of the quasi-stationary component C, coincides with the estimated time at which a superluminal blob ejected from the radio core (which caused the brightest flare of 2010) collides with the quasi-stationary component (at a projected distance of $\sim4.6$ pc from the radio core). The spectral index different behavior in the first ($5000 < \text{JD}-2450000 < 5600$) and second ($6600 < \text{JD}-2450000 < 7900$) flaring periods suggest changes in the physical conditions. The complex nature of the second period can be a result of a superposition of multiple events at different locations. The Mg~II has an anti-correlation with the UV-continuum while Fe~II correlates positively. Except by the time of the brightest flare of 2010, when both have a strong response at high continuum luminosities. Our results suggest that the dominant gamma-ray emission mechanism for the first flaring period is External Compton. For the second flaring period the seed photons emission region is co-spatial with the gamma-ray emission region. However, a SED study using a multizone jet emission model is required to confirm the nature of each significant flare during the second period.

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