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arXiv 1902.05237astro-ph.SR
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冷却回路系统中的等离子体流动

Plasma flows in the cool loop systems

Yamini K. Rao, Abhishek K. Srivastava, Pradeep Kayshap, Klaus Wilhelm, Bhola N. Dwivedi

摘要:

我们研究了三个数据集所观察到的界面区域成像光谱仪(IRIS)的低洼冷回路系统的动力学。利用光球层和过渡区(TR)之间形成的各种谱线,研究了观测到的冷环系统内部和周围的辐射、多普勒频移和谱线宽度。循环线的足迹点要么由蓝移或红移主导。各种环线蓝移足点上方速度的同空间变化显示出从Mg\,{ \sc ii} k线(2796.20~Å;地层温度:log(T/K)= 4.0)中的非常小的上升速度(-1至+1)km/s)到Si\,{ \sc iv}中的高上升速度(-10至-20)km/s)。因此,在位于Mg I,{\sc ii} k和Si I,{\sc iv}(1402.77 μ g; log(T/K)= 4.8)之间的谱线Cl,{\sc ii}(1334.53 μ g; \log(T/K)= 4.3)中的这些环系统的足点上方观察到等离子体流从红移(向下流动)到蓝移(向上流动)的转变。在所有三组观测数据中一致地观察到这种流动反转。回路系统的另一个足点始终保持红移,指示向下流动的血浆。本文采用多谱线谱线分析方法,详细描述了冷环系统中等离子体流动反转导致的质量输运及其形成过程。脉冲能量释放,由于小规模的重联以上的循环足点似乎是最有可能的原因突然启动的等离子体流明显在TR温度。

英文摘要:

We study the dynamics of low-lying cool loop systems for three datasets as observed by the Interface Region Imaging Spectrograph (IRIS). Radiances, Doppler shifts and line widths are investigated in and around observed cool loop systems using various spectral lines formed between the photosphere and transition region (TR). Footpoints of the loop threads are either dominated by blueshifts or redshifts. The co-spatial variation of velocity above the blue-shifted footpoints of various loop threads shows a transition from very small upflow velocities ranging from (-1 to +1) km/s in the Mg\,{\sc ii} k line (2796.20~Å; formation temperature: log (T/K) = 4.0) to the high upflow velocities from (-10 to -20) km/s in Si\,{\sc iv}. Thus, the transition of the plasma flows from red-shift (downflows) to the blue-shift (upflows) is observed above the footpoints of these loop systems in the spectral line C\,{\sc ii} (1334.53~Å; \log (T/K) = 4.3) lying between Mg\,{\sc ii} k and Si\,{\sc iv} (1402.77~Å; log (T / K) = 4.8). This flow inversion is consistently observed in all three sets of the observational data. The other footpoint of loop system always remains red-shifted indicating downflowing plasma. The multi-spectral line analysis in the present paper provides a detailed scenario of the plasma flows inversions in cool loop systems leading to the mass transport and their formation. The impulsive energy release due to small-scale reconnection above loop footpoint seems to be the most likely cause for sudden initiation of the plasma flows evident at TR temperatures.

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