日冕亮点的色球成分

M. Madjarska, J. Chae, F. Moreno-Insertis, Zhenyong Hou, D. Nóbrega-Siverio, Hannah Kwak, K. Galsgaard, Kyuhyoun Cho
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引用次数: 7

摘要

我们研究了构成日冕亮点(CBP)的小尺度日冕环的色球对应物及其对光球磁通量增加伴随共时CBP加热的响应。我们使用了来自AIA和HMI/SDO的联合观测数据,以及快速成像太阳光谱仪在Halpha和caii 8542线上拍摄的数据。我们使用了一种新的多层光谱反演技术来推导出半环温度的时间变化。我们发现,在色球温度下,CBP的对应物是由一束黑暗细长的特征组成的,在这项工作中被称为“阿尔法环”,它构成了CBP环磁结构的一个组成部分。由于磁通的出现而引起的光球磁通量的增加伴随着CBP环的日冕辐射的增加,这是一个加热事件。我们还观察到与新hl和斑点的发生有关的色球活性增强。虽然日冕辐射和磁通量的增加似乎是同时发生的,但CBP的Halpha对应体的响应发生在小于3分钟的小延迟中。在一个高通量点和一个CBP脚点发现,相对于事件前的值,温度急剧升高,估计为46%和55%,在日冕加热事件后也开始延迟小于3~min。低洼CBP环流结构在整个观测期内保持非电位。对上覆日冕的磁拓扑分析揭示了日冕零点在加热事件的开始和结束时的存在。CBP对应的色球响应的延迟表明加热可能发生在日冕高度。
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The chromospheric component of coronal bright points
We investigate the chromospheric counterpart of small-scale coronal loops constituting a coronal bright point (CBP) and its response to a photospheric magnetic-flux increase accompanied by co-temporal CBP heating. We used co-observations from the AIA and HMI/SDO, together with data from the Fast Imaging Solar Spectrograph taken in the Halpha and Ca II 8542 lines. We used a new multi-layer spectral inversion technique to derive the temporal variations of the temperature of the Halpha loops (HLs). We find that the counterpart of the CBP, as seen at chromospheric temperatures, is composed of a bundle of dark elongated features named in this work Halpha loops, which constitute an integral part of the CBP loop magnetic structure. An increase in the photospheric magnetic flux due to flux emergence is accompanied by a rise of the coronal emission of the CBP loops, that is a heating episode. We also observe enhanced chromospheric activity associated with the occurrence of new HLs and mottles. While the coronal emission and magnetic flux increases appear to be co-temporal, the response of the Halpha counterpart of the CBP occurs with a small delay of less than 3 min. A sharp temperature increase is found in one of the HLs and in one of the CBP footpoints estimated at 46% and 55% with respect to the pre-event values, also starting with a delay of less than 3~min following the coronal heating episode. The low-lying CBP loop structure remains non-potential for the entire observing period. The magnetic topological analysis of the overlying corona reveals the presence of a coronal null point at the beginning and towards the end of the heating episode. The delay in the response of the chromospheric counterpart of the CBP suggests that the heating may have occurred at coronal heights.
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