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The Recovery of CME-Related Dimmings and the ICME’s Enduring Magnetic Connection to the Sun

机译:与CME有关的调光的恢复以及ICME与太阳的持久磁性连接

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It is generally accepted that transient coronal holes (TCHs, dimmings) correspond to the magnetic footpoints of CMEs that remain rooted in the Sun as the CME expands out into the interplanetary space. However, the observation that the average intensity of the 12 May 1997 dimmings recover to their pre-eruption intensity in SOHO/EIT data within 48 hours, whilst suprathermal unidirectional electron heat fluxes are observed at 1 AU in the related ICME more than 70 hours after the eruption, leads us to question why and how the dimmings disappear whilst the magnetic connectivity is maintained. We also examine two other CME-related dimming events: 13 May 2005 and 6 July 2006. We study the morphology of the dimmings and how they recover. We find that, far from exhibiting a uniform intensity, dimmings observed in SOHO/EIT data have a deep central core and a more shallow extended dimming area. The dimmings recover not only by shrinking of their outer boundaries but also by internal brightenings. We quantitatively demonstrate that the model developed by Fisk and Schwadron (Astrophys. J. 560, 425, 2001) of interchange reconnections between “open” magnetic field and small coronal loops is a strong candidate for the mechanism facilitating the recovery of the dimmings. This process disperses the concentration of “open” magnetic field (forming the dimming) out into the surrounding quiet Sun, thus recovering the intensity of the dimmings whilst still maintaining the magnetic connectivity to the Sun.
机译:人们普遍认为,瞬变的日冕孔(TCHs,变暗)对应于CME扩展到行星际空间时仍然植根于太阳中的CME的磁性脚点。但是,观察到1997年5月12日的暗光的平均强度在48小时内恢复到SOHO / EIT数据中的喷发前强度,而相关ICME在超过70小时后于1 AU观测到超热单向电子热通量。喷发使我们质疑为什么在保持磁连通性的同时调光为什么消失以及如何消失。我们还研究了其他两个与CME相关的调光事件:2005年5月13日和2006年7月6日。我们研究了调光的形态及其恢复方式。我们发现,SOHO / EIT数据中观察到的调光远没有表现出均匀的强度,而是具有较深的中心核心和较浅的扩展调光区域。调光不仅可以通过缩小其外部边界来恢复,还可以通过内部增亮来恢复。我们定量地证明了由Fisk和Schwadron(Astrophys。J. 560,425,2001)开发的“开放”磁场与小的冠状环之间的互换重新连接的模型对于促进调光的机理是一个强有力的候选者。此过程将“开放”磁场(形成调光)的浓度分散到周围的安静太阳中,从而恢复了调光的强度,同时仍保持与太阳的磁连通性。

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