论文标题

改进的伽马射线二进制二进制解决方案1FGL J1018.6-5856

Improved binary solution for the gamma-ray binary 1FGL J1018.6-5856

论文作者

van Soelen, B., Keague, S. Mc, Malyshev, D., Chernyakova, M., Komin, N., Matchett, N., Monageng, I. M.

论文摘要

伽马射线二进制1FGL J1018.6-5856由O6V((F))型星和未知的紧凑型物体组成,并显示从无线电到非常高的能量伽马射线的轨道调制发射。 X射线灯曲线显示与GEV发射相同的阶段的最大值,但在阶段$ ϕ = 0.2-0.6 $之间的次级最大值。对二元系统的明确解决方案对于理解系统内发生的排放机制很重要。为了改善现有的二进制解决方案,我们使用南部非洲大型望远镜对光学伴侣进行了径向速度测量,并分析了公开可用的X射线和GEV伽马射线数据。在费米 - 拉特数据中搜索周期性的轨道周期为$ p = 16.5507 \ pm0.0004 $ d。在这个新时期举行的径向速度的最佳拟合解决方案发现,该系统比以前的观察值更古怪,$ e = 0.531 \ pm 0.033 $,其经度的periastron为$ 151.2 \ pm 5.1^\ circ $,并且质量更大,质量更大$ f = 0.00432 \ pm 0.00432 \ pm 0.0007 $ $ $ $ $ $ $ y_我们提出,X射线和伽马射线光曲线围绕0阶段0的峰值是由于观察到指向观察者的Pulsar和恒星风之间形成的密闭冲击。 X射线通量在0.25-0.75处的次级增加或强烈的快速变化是由于多个随机定向的恒星风团/脉冲星风相互作用,围绕Apastron周围的相互作用。

The gamma-ray binary 1FGL J1018.6-5856 consists of an O6V((f)) type star and an unknown compact object, and shows orbitally modulated emission from radio to very high energy gamma rays. The X-ray light curve shows a maximum around the same phase as the GeV emission, but also a secondary maximum between phases $ϕ=0.2 - 0.6$. A clear solution to the binary system is important for understanding the emission mechanisms occurring within the system. In order to improve on the existing binary solution, we undertook radial velocity measurements of the optical companion using the Southern African Large Telescope, as well as analysed publicly available X-ray and GeV gamma-ray data. A search for periodicity in Fermi-LAT data found an orbital period of $P=16.5507\pm0.0004$ d. The best fit solution to the radial velocities, held at this new period, finds the system to be more eccentric than previous observations, $e=0.531 \pm 0.033$ with a longitude of periastron of $151.2 \pm 5.1^\circ$, and a larger mass function $f = 0.00432\pm 0.00077$ M$_\odot$. We propose that the peaks in the X-ray and gamma-ray light curves around phase 0 are due to the observation of the confined shock formed between the pulsar and stellar wind pointing towards the observer. The secondary increase or strong rapid variations of the X-ray flux at phases 0.25-0.75 is due to the interaction of multiple randomly oriented stellar wind clumps/pulsar wind interactions around apastron.

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