The EUV spectrum of the Sun: SOHO CDS NIS radiances during solar cycle 23

The EUV spectrum of the Sun: SOHO CDS NIS radiances during solar cycle 23
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太阳的 EUV 光谱:太阳周期期间的 SOHO CDS NIS 辐射率 23

DOI:
10.1051/0004-6361/201322841
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发表时间:
2014
影响因子:
6.5
通讯作者:
Andretta V
Andretta V
中科院分区:
物理与天体物理2区
文献类型:
--
作者:
Andretta V

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首次提出并讨论了太阳过渡区和日冕在一个太阳活动周期内的极紫外辐射。这些测量是在1996年至2010年期间使用SOHO/日冕诊断光谱仪(CDS)获得的。我们发现,边缘增亮显着影响任何表征的太阳辐射。我们提出的肢体增亮功能的主线,并发现它不会改变可测量的周期。我们证实了先前的研究结果,即辐射直方图的冷却线有一个很好的定义,对数正态安静的太阳组件,虽然我们的结果不同于以前的。最低辐射率对数正态分布的宽度沿周期沿着是恒定的。中心到边缘的变化和辐射统计分布的分析都指向一个恒定的安静的太阳发射沿着太阳活动周期23。在1 MK以上形成的谱线会受到活跃区域的显著影响,事实上,在最大活动期间,没有“安静的太阳”区域可以被定义。在低于1.5 MK下形成的线中的大部分辐照度变化是由于发射区域的变化。对于较热的线,发射面积饱和到几乎100%的全太阳盘在最大的活动,而同时由于活动区域的排放增加了一个数量级以上。我们发现,活跃地区周围的结构,有时被称为黑暗的晕或黑暗的檐篷,是常见的,并讨论他们的相似性和差异与冕洞。特别是,我们展示了它们如何在TR线中清晰可见,这与日冕洞相反。
For the first time, we present and discuss EUV radiances of the solar transition region (TR) and corona obtained during a solar cycle. The measurements were obtained with the SOHO/coronal diagnostic spectrometer (CDS) during the period from 1996 to 2010. We find that limb-brightening significantly affects any characterisation of the solar radiances. We present the limb-brightening function for the main lines and find that it does not change measurably during the cycle. We confirm earlier findings that the radiance histogram of the cooler lines have a well defined, log-normal quiet-Sun component, although our results differ from previous ones. The width of the lowest-radiance log-normal distribution is constant along the cycle. Both the analysis of the centre-to-limb variation and of the radiance statistical distribution point to a constant quiet Sun emission along solar cycle 23. Lines formed above 1 MK are dramatically affected by the presence of active regions, and indeed, no “quiet Sun” region can be defined during periods of maximum activity. Much of the irradiance variability in lines formed below 1.5 MK is due to a change in the emitting area. For hotter lines, the emitting area saturates to almost 100% of full solar disk at the maximum of activity, while simultaneously the emission due to active regions increases by more than an order of magnitude. We show that structures around active regions, sometimes referred to as dark halos or dark canopies, are common and discuss their similarities and differences with coronal holes. In particular, we show how they are well visible in TR lines, contrary to coronal holes.
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