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arXiv 2003.01999astro-ph.HE
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2015年6月平谱射电类星体3C 279耀斑的Gamma-ray和光学性质

Gamma-ray and Optical properties of the flat spectrum radio quasar 3C 279 flare in June 2015

K K Singh, P J Meintjes, B Bisschoff, F A Ramamonjisoa, B van Soelen

摘要:

平谱射电类星体3C 279在2015年6月16日(MJD 57189)处于极高的活动状态。在本文中,我们使用2015年6月1日至30日期间(MJD 57174-57203)的\emph{Fermi} -LAT,SMARTS和SPOL观测数据研究了高能$γ$射线和光学波段中的耀斑事件的特性。由\emph{Fermi} -LAT探测到的$γ$ -射线带中的最高发射状态显示出$\sim$ 2 $\times$ 10 $^{-7}$ erg~cm $^{-2}$ ~s $^{-1}$的峰值通量,这是在源的低活性状态下测量的通量水平的25倍以上.每日\emph{Fermi} -LAT光变曲线的时间分析表明,巨大的耀斑发作的特征上升和衰减时间小于一天。B、V、R和J波段的光学日光变曲线也表明3C 279的耀斑活动,其通量水平在2015年6月16日至17日达到峰值(MJD 57189-57190)。离散相关函数分析表明,在耀斑发作期间,$γ$射线峰和光学峰之间存在1天或更长的时滞。还观察到$γ$射线发射显示出更硬时更亮的行为,而光学发射则表现出相反的行为。观测到耀斑期间的$γ$射线发射区域非常紧凑,并且靠近喷流的底部。在此期间使用SPOL测量的500-700 nm波长范围内的线偏振度也是高度可变的,在$γ$射线耀斑后一天具有$\sim$ 30 $\%$的峰值。在$γ$射线耀斑期间,几乎同时发生的$γ$射线通量点与偏振度呈线性反相关。线偏振度的显著下降表明发射区中缠结的磁场强度突然增加。

英文摘要:

The flat spectrum radio quasar 3C 279 was observed in an extremely high activity state on June 16, 2015 (MJD 57189). In this paper, we investigate the properties of this flaring episode in the high energy $γ$-ray and optical bands using data from the \emph{Fermi}-LAT, SMARTS, and SPOL observations during the period June 1-30, 2015 (MJD 57174-57203). The highest emission state in the $γ$-ray band detected by the \emph{Fermi}-LAT exhibits a peak flux of $\sim$ 2$\times$10$^{-7}$ erg~cm$^{-2}$~s$^{-1}$ which is more than 25 times the flux level measured in the low activity state of the source. The temporal analysis of the daily \emph{Fermi}-LAT light curve suggests that the giant flaring episode has characteristic rise and decay times less than one day. The optical daily light curves in B, V, R, and J bands also indicate the flaring activity from 3C 279 with flux levels peaking for two days on June 16-17, 2015 (MJD 57189-57190). The discrete correlation function analysis indicates a time lag of 1 day or longer between the $γ$-ray and optical peaks during the flaring episode. The $γ$-ray emission is also observed to show a harder-when-brighter behaviour whereas optical emission exhibits an opposite behaviour. The $γ$-ray emission region during the flare is observed to be very compact and is located close to the base of the jet. The degree of linear polarization in the wavelength range 500-700 nm measured using SPOL during this period is also highly variable with a peak of $\sim$ 30$\%$ one day after the $γ$-ray flare. Near simultaneous $γ$-ray flux points show a linear anti-correlation with the degree of polarization during the period of $γ$-ray flare. The significant drop in the degree of linear polarization suggests a sudden increase in the tangled magnetic field strength in the emission region.

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