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首页> 外文期刊>The Astrophysical journal >EXTREMELY HIGH POLARIZATION IN THE 2010 OUTBURST OF BLAZAR 3C 454.3
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EXTREMELY HIGH POLARIZATION IN THE 2010 OUTBURST OF BLAZAR 3C 454.3

机译:Blazar 3C 454.3在2010年爆发时的极高极化

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摘要

The gamma-ray-detected blazar 3C 454.3 exhibits dramatic flux and polarization variations in the optical and near-infrared bands. In 2010 December, the object emitted a very bright outburst. We monitored it for approximately four years (including the 2010 outburst) by optical and near-infrared photopolarimetry. During the 2010 outburst, the object emitted two rapid, redder brightenings, at which the polarization degrees (PDs) in both bands increased significantly and the bands exhibited a frequency-dependent polarization. The observed frequency-dependent polarization leads us to propose that the polarization vector is composed of two vectors. Therefore, we separate the observed polarization vectors into short- and long-term components that we attribute to the emissions of the rapid brightenings and the outburst that varied the timescale of days and months, respectively. The estimated PD of the short-term component is greater than the maximum observed PD and is close to the theoretical maximum PD. We constrain the bulk Lorentz factors and inclination angles between the jet axis and the line of sight from the estimated PDs. In this case, the inclination angle of the emitting region of short-term component from the first rapid brightening should be equal to 90°, because the estimated PD of the short-term component was approximately equal to the theoretical maximum PD. Thus, the Doppler factor at the emitting region of the first rapid brightening should be equal to the bulk Lorentz factor.
机译:伽马射线检测的blazar 3C 454.3在光学和近红外波段显示出显着的通量和偏振变化。在2010年12月,该物体发出了非常明亮的爆发。我们通过光学和近红外光偏振法对它进行了大约四年(包括2010年的爆发)的监测。在2010年爆发期间,该物体发出了两个快速的红色增亮,这两个波段的偏振度(PDs)显着增加,并且这些波段表现出与频率相关的偏振。观察到的频率相关极化导致我们提出极化向量由两个向量组成。因此,我们将观测到的极化矢量分为短期和长期两个部分,我们将其归因于快速增亮的发射和爆发,分别改变了几天和几个月的时间尺度。短期分量的估计PD大于观察到的最大PD,并且接近理论上的最大PD。我们根据估计的局部放电来约束总体洛伦兹因子和射流轴与视线之间的倾斜角度。在这种情况下,由于短期分量的估计PD近似等于理论上的最大PD,因此从第一次快速增亮起,短期分量的发射区域的倾斜角应等于90°。因此,在第一快速增亮的发射区域处的多普勒因子应等于体洛伦兹因子。
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