论文标题
连续的无点磁重新连接建立一个圆环不稳定的磁通绳,触发X9.3 X9.3太阳能活动区域〜12673
Continuous Null-Point Magnetic Reconnection Builds Up a Torus Unstable Magnetic Flux Rope Triggering the X9.3 Flare in Solar Active Region~12673
论文作者
论文摘要
2017年9月6日从活跃地区NOAA 12673发生了两次X级太阳能耀斑:第一个是约束的X2.2耀斑,仅遵循$ \ sim 3 $ 3 $ 3 $ 3 $ 3 $ 3 $,第二个是太阳能周期24中最强的耀斑,达到了X9.3级别,达到了X9.3级别,并伴有冠状质量弹药折射。为什么这两种X级耀斑以相似的磁性构型出现在同一位置,而一个是爆发的,而另一个则不是呢?在这里,我们通过非线性磁场的外推从具有高节奏的矢量磁图的时间顺序跟踪冠状磁场演化。对磁场的详细分析表明,磁通绳(MFR)形成并逐渐生长在第一次耀斑之前,此后不久,MFR的生长显着增强,高度的上升速度更快,远低于远低于曲曲线不稳定性的阈值,而磁性扭转只会略微增加。结合了EUV的观测和磁场外推,我们发现上覆的MFR是一个空点的磁性拓扑,在第一次耀斑之后可以看到复发的亮度。因此,我们提出了一种解释两种耀斑发生的情况。第一次耀斑发生是自MFR达到足够高的高度以激活空点的高度,并且其连续的膨胀迫使无点重新连接。这种重新连接削弱了上覆的场,使MFR的上升速度更快,最终越过了圆环不稳定性的阈值,并触发了第二个爆发耀斑。
Two X-class solar flares occurred on 2017 September 6 from active region NOAA 12673: the first one is a confined X2.2 flare, and it is followed only $\sim 3$ hours later by the second one, which is the strongest flare in solar cycle 24, reaching X9.3 class and accompanied with a coronal mass ejection. Why these two X-class flares occurred in the same position with similar magnetic configurations, but one is eruptive while the other is not? Here we track the coronal magnetic field evolution via nonlinear force-free field extrapolations from a time sequence of vector magnetograms with high cadence. A detailed analysis of the magnetic field shows that a magnetic flux rope (MFR) forms and grows gradually before the first flare, and shortly afterwards, the MFR's growth is significantly enhanced with a much faster rise in height, from far below the threshold of torus instability to above it, while the magnetic twist only increases mildly. Combining EUV observations and the magnetic field extrapolation, we found that overlying the MFR is a null-point magnetic topology, where recurrent brightening is seen after the first flare. We thus suggest a scenario to interpret the occurrence of the two flares. The first flare occurred since the MFR reached a high enough height to activate the null point, and its continuous expansion forces the null-point reconnection recurrently. Such reconnection weakens the overlying field, allowing the MFR to rise faster, which eventually crosses the threshold of torus instability and triggers the second, eruptive flare.