SPATIAL AND TEMPORAL VARIATIONS OF K Ca II LINE PROFILE SHAPES IN DIFFERENT STRUCTURES OF THE SOLAR CHROMOSPHERE. II. DETERMINATION TECHNIQUE AND CORRELATION RELATIONSHIPS BETWEEN THE K CA II LINE PARAMETERS FOR K1 AND K2 FEATURES

I. Turova, S. Grigoryeva, O. Ozhogina
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引用次数: 1

Abstract

We have studied two regions located at the base of a coronal hole. For the K₁ intensity minima and K₂ peaks, which form between the upper photosphere and the lower chromosphere and in the lower chromosphere respectively, a number of Ca II line parameters have been computed. We have improved the determination technique for ∆λᴋ₁ᵥ and ∆λᴋ₁ᵣ, ∆λᴋ₂ᵥ and ∆λᴋ₂ᵣ line profile shifts, including certain cases when their direct determination was complicated. We have determined Iᴋ₁ᵥ, Iᴋ₁ᵣ, Iᴋ₂ᵥ, Iᴋ₂ᵣ intensities, K₁ minima and K₂ peaks separations SEPᴋ₁ = ∆λᴋ₁ᵣ – ∆λᴋ₁ᵥ, SEPᴋ₂ = ∆λᴋ₂ᵣ – ∆λᴋ₂ᵥ, respectively. We have constructed scatter plots and have computed correlation relationships between parameters relating to different levels of atmosphere. We have obtained the following results. The intensities observed in the lower and middle chromosphere are connected closer than intensities related to the upper photosphere and middle chromosphere. The structures with a stronger magnetic field are brighter at the upper photosphere and lower chromosphere levels as compared to the structures with a weaker magnetic field. K₁ minima separations are of greater value for the structures with a stronger magnetic field relative to the structures with a weaker magnetic field, whereas K₂ peaks separations demonstrate the opposite behavior. They are lower for the structures with a stronger magnetic field. It is true not only for the chosen structures belonging to quiet regions but also for the plage, though we need additional statistics for plages. The relation between shifts of K₁ minima and K₂ peak intensities for violet and red wings appeared to be weak. This may be due to the considerable contribution of random movements to the velocity field at the upper photosphere and lower chromosphere levels or due to different forming levels for the profile violet and red wings.
太阳色球不同结构中K - Ca - II线轮廓的时空变化。2k1和k2特征的k - ca - ii线参数测定技术及相关关系
我们研究了位于日冕洞底部的两个区域。对于分别形成于上光球与下色球之间和下色球内的K₁强度极小值和K₂峰,计算了若干Ca II线参数。我们改进了∆λ k₁ᵥ和∆λ k₁ᵣ,∆λ k₂ᵥ和∆λ k₂ᵣ线剖面移位的测定技术,包括其直接测定复杂的某些情况。我们已经确定我ᴋ₁ᵥ,我ᴋ₁ᵣ,我ᴋ₂ᵥ,我ᴋ₂ᵣ强度,K₁最小值和K₂峰分离9月ᴋ₁=∆λᴋ₁ᵣ——∆λᴋ₁ᵥ,9月ᴋ₂=∆λᴋ₂ᵣ——∆λᴋ₂ᵥ,分别。我们构建了散点图,并计算了与不同大气水平有关的参数之间的相关关系。我们得到了以下结果。在中下色球层观测到的光强比在中上色球层观测到的光强联系更紧密。与磁场较弱的结构相比,磁场较强的结构在光球层的上层和色球层的下层较亮。相对于磁场较弱的结构,具有较强磁场的结构,K₁最小值分离具有更大的价值,而K₂峰值分离则表现出相反的行为。对于具有较强磁场的结构,它们更低。这不仅适用于属于安静区域的选定结构,也适用于斑块,尽管我们需要对斑块进行额外的统计。紫色翼和红色翼的K₁极小值位移与K₂峰强度之间的关系较弱。这可能是由于随机运动对上层光球层和下层色球层的速度场有相当大的贡献,或者是由于紫色和红色翼的轮廓形成水平不同。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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