论文标题

低电晕中冠状质量弹出的不对称扩张

Asymmetric expansion of coronal mass ejections in the low corona

论文作者

Cremades, Hebe, Iglesias, Francisco A., Merenda, Luciano A.

论文摘要

目标。对冠状质量弹出(CME)形态的研究是一种吉祥的方法,用于了解磁场在CME中的结构。尽管较早的研究表明,正交方向的CME宽度宽度不对称,但尚未使用多视点观测来对其进行检查。方法。我们检查了在观察航天器位置和CME轨迹的特定条件下发生的十二个CME的形态的早期进化(低于太阳半径),这有利于减少此处使用的3D重建涉及的不确定性。这些事件是通过前向建模工具仔细地重建的,使用立体声EUVI和SDO/AIA的同时观察为输入,当时在电晕中较低,然后在立体声和Soho Coronagraph的视野中随后随访。然后,我们检查由重建引起的形态参数的高度演变。结果。对这组CME的多观看分析表明,它们的最初膨胀 - 三个太阳半径 - 非常不对称且非自由相似。角度宽度,即沿着CME的主轴($ AW_L $)和正交方向($ AW_D $,代表通量绳直径),其高度较高的变化速率低于此高度,其增长率较高,其增长率为$ AW_L $,其高度大于$ AW_D $的高度,也低于该高度。沿CME的主轴的角度宽度平均是正交方向$ AW_D $的$ \ $ \ $ 1.8倍。两个膨胀速度的比率,即在CMES主轴的指示和正交的指示下,在$ \ sim $ 4 $ 4太阳能半径之后几乎是恒定的,平均比率为$ \ $ \ $ \ $ 1.6。定义宽度变化率稳定的高度对于$ AW_L $比$ aw_d $要大。

Aims. The study of the morphology of coronal mass ejections (CMEs) is an auspicious approach to understanding how magnetic fields are structured within CMEs. Although earlier studies have suggested an asymmetry in the width of CMEs in orthogonal directions, this has not been inspected using multi-viewpoint observations. Methods. We inspect the early evolution (below ten solar radii) of the morphology of a dozen CMEs occurring under specific conditions of observing spacecraft location and CME trajectory, favorable to reduce uncertainties typically involved in the 3D reconstruction used here. These events are carefully reconstructed by means of a forward modeling tool using simultaneous observations of STEREO EUVI and SDO/AIA as input when originating low in the corona, and followed up in the outer fields of view of the STEREO and the SOHO coronagraphs. We then examine the height evolution of the morphological parameters arising from the reconstructions. Results. The multi-viewpoint analysis of this set of CMEs revealed that their initial expansion --below three solar radii-- is considerably asymmetric and non-self-similar. Both angular widths, namely along the main axes of CMEs ($AW_L$) and in the orthogonal direction ($AW_D$, representative of the flux rope diameter), exhibit much steeper change rates below this height, with the growth rate of $AW_L$ found to be larger than that of $AW_D$, also below that height. Angular widths along the main axes of CMEs are on average $\approx$1.8 times larger than widths in the orthogonal direction $AW_D$. The ratios of the two expansion speeds, namely in the directions of CMEs main axes and in their orthogonal, are nearly constant in time after $\sim$4 solar radii, with an average ratio $\approx$1.6. Heights at which the width change rate is defined to stabilize are greater for $AW_L$ than for $AW_D$.

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