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arXiv 0710.0247astro-ph
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Ca { \small{II} } 8662晶体中动态纤维的光谱测量

Spectroscopic measurements of dynamic fibrils in the Ca {\small{II}} 8662 Å line

Oystein Langangen, Mats Carlsson, Luc Rouppe van der Voort, Viggo Hansteen, Bart De Pontieu

摘要:

我们提出了高空间分辨率的光谱测量的动态纤维(DF)的Ca { \small{II} } 8662线。这些数据显示了所识别的DF中的清晰多普勒频移,这表明至少DF的子集是色球层中的实际质量运动。对26个DF的统计分析揭示了最大速度和减速度之间的强的和统计上显著的相关性。的速度和减速的范围是大大降低,约一个因素,在我们的光谱观测相比,早期的结果基于适当的运动在窄带图像。不同的观测方法有着根本的区别;当用光谱法观测DF时,测得的多普勒频移是大气速度的结果,用扩展高度上的速度响应函数加权。当在窄带图像中观察到DF的自行时,观察到DF顶部的移动。由于DF和周围环境之间的高对比度,该点被清晰地限定。两种方法之间的观测差异进行了研究,通过几个数值实验,使用数值模拟和窄带H $α$图像的时间序列。在模拟的基础上,我们得出结论,较低的最大速度是由低的形成高度的钙IR线。我们的结论是,目前的观察结果支持早期的结果,即DF驱动的磁声冲击所激发的对流和p模式。

英文摘要:

We present high spatial resolution spectroscopic measurements of dynamic fibrils (DFs) in the Ca {\small{II}} 8662 Å line. These data show clear Doppler shifts in the identified DFs, which demonstrates that at least a subset of DFs are actual mass motions in the chromosphere. A statistical analysis of 26 DFs reveals a strong and statistically significant correlation between the maximal velocity and the deceleration. The range of the velocities and the decelerations are substantially lower, about a factor two, in our spectroscopic observations compared to the earlier results based on proper motion in narrow band images. There are fundamental differences in the different observational methods; when DFs are observed spectroscopically the measured Doppler shifts are a result of the atmospheric velocity, weighted with the response function to velocity over an extended height. When the proper motion of DFs is observed in narrow band images, the movement of the top of the DF is observed. This point is sharply defined because of the high contrast between the DF and the surroundings. The observational differences between the two methods are examined by several numerical experiments using both numerical simulations and a time series of narrow band H$α$ images. With basis in the simulations we conclude that the lower maximal velocity is explained by the low formation height of the Ca IR line. We conclude that the present observations support the earlier result that DFs are driven by magneto-acoustic shocks exited by convective flows and p-modes.

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