论文标题

Magnetar SGR 1830-0645爆发的X射线爆发和持续的排放特性

X-ray burst and persistent emission properties of the magnetar SGR 1830-0645 in outburst

论文作者

Younes, G., Hu, C. -P., Bansal, K., Ray, P. S., Pearlman, A. B., Kirsten, F., Wadiasingh, Z., Gogus, E., Baring, M. G., Enoto, T., Arzoumanian, Z., Gendreau, K. C., Kouveliotou, C., Guver, T., Harding, A. K., Majid, W. A., Blumer, H., Hessels, J. W. T., Gawronski, M. P., Bezrukovs, V., Orbidans, A.

论文摘要

我们报告了磁盘SGR 1830-0645的X射线监测,涵盖了2020年10月爆发后223天,以及Chandra和无线电观察结果。我们介绍了到目前为止来源最准确的自旋胚层:$ν= 0.096008680(2)$ 〜Hz,$ \dotν= -6.2(1)\ times10^{ - 14} $ 〜Hz〜s $^s $^s $^{ - 1} $,以及一个重要的第二和第三频率派生术语和第三个频率的指示噪音。在整个活动中,相平均0.8--7〜KEV频谱非常适合双黑体(BB)模型。 BB温度在0.46和1.2 KEV处保持恒定。每个组件的面积和通量降低了6倍,最初是通过陡峭的衰减趋势持续约46天,然后是浅长期。相同能量范围内的脉冲形状最初是复杂的,表现出三个不同的峰,但在整个爆发过程中都具有清晰的连续演化,朝着更简单的单脉冲形状。 RMS脉冲分数很高,从约40%增加到50%。我们发现脉冲形状或分数对能量的依赖性。这些结果表明,在爆发发作时出现了多个可能具有温度梯度的热点,并且随着爆发的衰落而缩水。我们检测到84个微弱的爆发,\更好,在第一次在如此大的爆发样品中检测到这种现象时,最大程度地偏爱接近表面发射脉冲。这可能意味着爆发发射区域的高度非常低,并且触发机制连接到表面活性区。最后,我们在几个时期的无线电观察结果和多个频率没有发现脉冲或爆发样无线电发射的证据。

We report on NICER X-ray monitoring of the magnetar SGR 1830-0645 covering 223 days following its October 2020 outburst, as well as Chandra and radio observations. We present the most accurate spin ephemerides of the source so far: $ν=0.096008680(2)$~Hz, $\dotν=-6.2(1)\times10^{-14}$~Hz~s$^{-1}$, and a significant second and third frequency derivative terms indicative of non-negligible timing noise. The phase-averaged 0.8--7~keV spectrum is well fit with a double-blackbody (BB) model throughout the campaign. The BB temperatures remain constant at 0.46 and 1.2 keV. The areas and flux of each component decreased by a factor of 6, initially through a steep decay trend lasting about 46 days followed by a shallow long-term one. The pulse shape in the same energy range is initially complex, exhibiting three distinct peaks, yet with clear continuous evolution throughout the outburst towards a simpler, single-pulse shape. The rms pulsed fraction is high and increases from about 40% to 50%. We find no dependence of pulse shape or fraction on energy. These results suggest that multiple hotspots, possibly possessing temperature gradients, emerged at outburst-onset, and shrank as the outburst decayed. We detect 84 faint bursts with \nicer, having a strong preference for occurring close to the surface emission pulse maximum the first time this phenomenon is detected in such a large burst sample. This likely implies a very low altitude for the burst emission region, and a triggering mechanism connected to the surface active zone. Finally, our radio observations at several epochs and multiple frequencies reveal no evidence of pulsed or burst-like radio emission.

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