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arXiv 2302.08457astro-ph.SR
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色球纤维的温度诊断

Temperature diagnostics of chromospheric fibrils

M. Kriginsky, R. Oliver, D. Kuridze

AI总结:

本研究利用Ca II 854.2 nm和Mg II h & k谱线观测及反演技术诊断色球纤维热力学结构,发现纤维足点温度比中点高约300 K且呈对称变化,并指出单一Ca II谱线对温度响应不足,需结合多谱线才能准确推断其热力学性质。

摘要:

背景。色球纤维是连接附近相反极性光球磁场集中区域的细长结构。目标。我们评估使用现有仪器和反演技术推断色球纤维热力学结构的可能性与 drawbacks。方法。我们使用了瑞典 1 米太阳望远镜上的 CRISP 仪器获取的 Ca II 854.2 nm 线光谱观测数据,并与 IRIS 卫星观测的紫外 Mg II h & k 线协调进行。我们研究了这些色球谱线对温度的敏感性,以使用 Stockholm inversion Code 正确反演其光谱轮廓,并确定视场中手动追踪的色球纤维的温度、视线速度和微湍流速度。结果。纤维状结构显示出其温度沿长度位置非常特殊的依赖关系。它们在探测到的足点处的温度平均比中点高 300 K。温度变化在形状上几乎对称,部分追踪的纤维显示出类似的温度变化趋势。此外,对于纤维区域的大气反演模型,Ca II 854.2 nm 线核对温度变化的响应似乎不足以正确解析上述温度结构。只有添加更多对温度敏感的谱线(如 Mg II h & k 线)才能正确推断色球纤维的热力学性质。将此处获得的结果与之前针对明亮 Ca II K 纤维的研究进行比较,发现这些结构在温度方面具有极大的相似性。

英文摘要:

Context. Chromospheric fibrils are thin and elongated structures that connect nearby photospheric magnetic field concentrations of opposite polarities. Aims. We assess the possibilities and drawbacks related to the use of current instrumentation and inversion techniques to infer the thermodynamic structure of chromospheric fibrils. Methods. We employed spectroscopic observations obtained in the Ca ii 854.2 nm line with the CRISP instrument at the Swedish 1-m Solar Telescope and in coordination with observations in the ultraviolet Mg ii h & k lines taken with the IRIS satellite. We studied the temperature sensitivity of these chromospheric lines to properly invert their spectral profiles with the Stockholm inversion Code and determine the temperature, line-of-sight velocity, and microturbulent velocity of manually traced chromospheric fibrils present in the field of view. Results. Fibril-like structures show a very particular dependence of their temperature as a function of the position along their length. Their temperatures at the detected footpoints are, on average, 300 K higher than the temperature at the midpoint. The temperature variation appears to be almost symmetrical in shape, with partially traced fibrils showing a similar trend for the temperature variation. Additionally, the response of the Ca ii 854.2 nm line core to variations of the temperature for the inverted models of the atmosphere in fibril areas seems to be insufficient to properly resolve the aforementioned temperature structure. Only the addition of more temperature sensitive lines such as the Mg ii h & k lines would make it possible to properly infer the thermodynamic properties of chromospheric fibrils. Comparisons between the results obtained here and in previous studies focused on bright Ca ii K fibrils yield great similarities between these structures in terms of their temperature.

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