论文标题

利物浦 - 米达纳克(Liverpool-Maidanak)对爱因斯坦十字架(Einstein Cross)的监测2006年$ - $ 2019。 I. $ gvrri $光带和微透镜签名的光曲线

Liverpool-Maidanak monitoring of the Einstein Cross in 2006$-$2019. I. Light curves in the $gVrRI$ optical bands and microlensing signatures

论文作者

Goicoechea, L. J., Artamonov, B. P., Shalyapin, V. N., Sergeyev, A. V., Burkhonov, O. A., Akhunov, T. A., Asfandiyarov, I. M., Bruevich, V. V., Ehgamberdiev, S. A., Shimanovskaya, E. V., Zheleznyak, A. P.

论文摘要

Quasar Microlensing提供了一个独特的机会,可以解决遥远活跃的银河系核中的微小来源,并研究透镜星系中的紧凑物体种群。因此,我们使用4374利物浦望远镜和1.5 M Maidanak望远镜使用的4374光学框架搜索了重力诱导的重力镜头QSO QSO QSO QSO 2237+0305(Einstein Cross)的可变性。这些在2006年$ -2019期间的$ gvrri $框架经过均匀处理,以生成四个类星体图像A-D的准确的长期多波段光曲线。通过差异光曲线,我们发现了强烈的微透镜特征。然后,我们专注于图像C中两个推定的苛性腐蚀性事件的分析建模,发现了令人信服的证据,表明该图像经历了双重苛性速度。此外,我们的总体结果表明,当发射波长增加时,标准积分盘对紫外线连续发射源的亮度概况和源半径的增长相当好:$r_λ\ proptoλ^α$,$α$ = 1.33 $ \ pm $ 0.09。但是,我们警告说,在紫外线排放方案中得出企业结论之前,需要进行数值微透镜模拟,因为在第一个苛性菜交叉期间的$ vri $ band监视,并且我们的两个$α$指标之一导致了一些$α\ $α\ $ 1的好解决方案。

Quasar microlensing offers a unique opportunity to resolve tiny sources in distant active galactic nuclei and study compact object populations in lensing galaxies. We therefore searched for microlensing-induced variability of the gravitationally lensed quasar QSO 2237+0305 (Einstein Cross) using 4374 optical frames taken with the 2.0 m Liverpool Telescope and the 1.5 m Maidanak Telescope. These $gVrRI$ frames over the 2006$-$2019 period were homogeneously processed to generate accurate long-term multi-band light curves of the four quasar images A-D. Through difference light curves, we found strong microlensing signatures. We then focused on the analytical modelling of two putative caustic-crossing events in image C, finding compelling evidence that this image experienced a double caustic crossing. Additionally, our overall results indicate that a standard accretion disc accounts reasonably well for the brightness profile of UV continuum emission sources and for the growth in source radius when the emission wavelength increases: $R_λ \propto λ^α$, $α$ = 1.33 $\pm$ 0.09. However, we caution that numerical microlensing simulations are required before firm conclusions can be reached on the UV emission scenario because the $VRI$-band monitoring during the first caustic crossing and one of our two $α$ indicators lead to a few good solutions with $α\approx$ 1.

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