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Non-Maxwellian Redistribution in Solar Coronal Lyα Emission

机译:太阳日冕Lyα发射中的非麦克斯韦分布。

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This paper presents theoretical models of H I Lyα emission from the extended solar corona, taking into account various plasma kinetic effects that induce departures from Maxwellian velocity distributions. Such phenomena as suprathermal tails, strong temperature anisotropies, and skewed or double-peaked distributions have been observed in the solar wind, and UV spectroscopy is beginning to be able to detect their signatures in the corona. For resonantly scattered lines like H I Lyα, most of the physics is contained in the frequency-dependent redistribution function. The dependence of this function on the local plasma parameters is presented analytically for four different non-Maxwellian distributions, and optically thin line intensities are computed for a representative model of the fast solar wind. Isotropic power-law "κ" tails in the velocity distribution should be detectable between 2 and 5 ? from line center. Although existing observations that appear to have broad tails do not resemble those arising from κ-distributions, their presence is still possible. Anisotropic bi-Maxwellian distributions affect line profile shapes and total intensities via both their parallel and perpendicular components, and it is important to include an accurate description of the photon redistribution for large anisotropies. Skewness caused by a Chapman-Enskog expansion in the conductive heat flux is detectable as a unique non-Gaussian profile shape, but other types of collisionally beamed or skewed distributions may not noticeably affect the emission lines.
机译:本文介绍了扩展的日冕产生H ILyα发射的理论模型,其中考虑了各种等离子体动力学效应,这些效应导致偏离麦克斯韦速度分布。在太阳风中已经观察到诸如超热尾部,强温度各向异性以及偏斜或双峰分布等现象,紫外线光谱法已经开始能够在日冕中检测其特征。对于像H ILyα这样的共振散射线,大多数物理学都包含在频率相关的重新分布函数中。对于四个不同的非麦克斯韦分布,通过解析给出了该函数对局部等离子体参数的依赖性,并为快速太阳风的代表性模型计算了光学上的细线强度。速度分布中的各向同性幂律“κ”尾部应在2到5之间?从线中心。尽管现有观察到的尾巴宽阔与κ分布所产生的尾巴并不相似,但它们的存在仍然是可能的。各向异性双麦克斯韦分布通过其平行和垂直分量影响线轮廓的形状和总强度,因此,重要的是要包括对大各向异性的光子重新分布的准确描述。可以将传导热通量中Chapman-Enskog扩展引起的偏斜检测为唯一的非高斯轮廓形状,但是其他类型的碰撞光束或偏斜分布可能不会明显影响发射线。

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