类克利桑特 "日光层对 Lyα 的吸收

Erick Powell, M. Opher, M. Kornbleuth, I. Baliukin, A. Michael, B. Wood, V. Izmodenov, Gábor Tóth, V. Tenishev
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摘要

Lyα 吸收剖面被用来探测天球和日光层对氢壁和日珥尾的吸收。利用日光层的磁流体动力学模型,我们可以比较模拟和观测到的 Lyα 剖面,以探测日光层内部和附近的中性氢。关于日光层是具有长长的 "彗星状 "尾巴还是短短的 "羊角状 "尾巴,一直存在争议。在这里,我们首次利用类蛇尾日光层对 Lyα 的吸收进行了研究。在边界条件完全相同的情况下,我们比较了 BU 模型和莫斯科模型,前者呈现出类似羊角风的尾巴,后者呈现出类似彗星的尾巴。BU模型和莫斯科模型对机头目标(α Cen和36 Oph)的Lyα剖面几乎完全相同。尾部目标(HD 35296)的 Lyα 曲线则有所不同。尽管羊角面包模型的日珥尾缩短了,但仍能看到明显的下风日珥鞘吸收,只是浅了 5%,偏移了 4 km s-1。这意味着不需要用加长的日珥尾模型来重现日珥鞘Lyα吸收观测结果。更精细的观测光栅也许可以解决这一偏移问题。此外,当使用比莫斯科模型更高的星际介质(ISM)中性密度和等离子体密度以及更低的磁场(∣B LISM∣ = 3.2 μG,α BV ≈ 40°)时,我们发现与观测到的 Lyα 剖面有更好的一致性。没有一个模型能同时在所有方向上显示出一致性。此外,我们还发现,在确定性最小的 ISM 条件下(n p,LISM、n H,LISM、T LISM、B LISM),B LISM 对氢壁结构和 Lyα 剖面的影响最大。
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Lyα Absorption in a “Croissant-like” Heliosphere
Lyα absorption profiles have been used to detect astrospheres and heliospheric absorption from the hydrogen wall and heliotail. Using magnetohydrodynamic models of the heliosphere, we can compare simulated to observed Lyα profiles to probe the neutral hydrogen within and near the heliosphere. There is an ongoing controversy whether the heliosphere has a long “comet-like” tail or a short “croissant-like” tail. Here we present the first Lyα absorption investigation using a croissant-like heliosphere. With identical boundary conditions we compare the BU model, which presents a croissant-like tail, and the Moscow model, which presents a comet-like tail. The BU and Moscow models present nearly identical Lyα profiles toward nose targets (α Cen and 36 Oph). Differences in Lyα profiles are shown toward the tail target (HD 35296). Despite the shortened heliotail of the croissant model, significant downwind heliosheath absorption is seen, just 5% shallower and shifted by 4 km s−1. This implies that an extended tail model is not required to reproduce the heliosheath Lyα absorption observations. Finer observation gratings may be able to resolve this shift. Additionally, when using higher interstellar medium (ISM) neutral and plasma densities and lower magnetic field (∣B LISM∣ = 3.2 μG, α BV ≈ 40°) than in the Moscow model, we find better agreement with observed Lyα profiles. None of the models presented show agreement in all directions simultaneously. Furthermore, we show that for the ISM conditions with the least certainty (n p,LISM, n H,LISM, T LISM, B LISM), B LISM has the most significant effect on the structure of the hydrogen wall and Lyα profiles.
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