与太阳风质子进入有关的月球尾流中的波激发

M. Nishino, Yoshifumi Saito, Y. Kasahara, Y. Omura, K. Hashimoto, T. Ono, H. Tsunakawa, F. Takahashi, M. Fujimoto
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摘要

近月空间环境的特征是沿太阳风(SW)流在夜侧形成等离子体空腔区域,称为月球尾流。由于月球阻挡了西南波等离子体流,尾迹区域比周围的西南波区域要脆弱得多。月球尾流的等离子体环境考虑如下:由于高能SW电子可以很容易地进入夜侧区域,而SW质子则不能,因此尾流区域应该带负电荷。月球尾流的富电子状态在尾流边界产生双极性(向内)电场,其中SW质子沿着遥远尾流的行星际磁场(IMF)逐渐来到尾流中心。与此同时,据报道,SW进入遥远的尾迹会产生等离子体波。宽频静电噪声(BEN)是由Wind航天器在遥远的尾迹(距离月球约1万公里)探测到的。由于双极电场加速/减速SW质子束进入尾迹,导致离子双流不稳定。这也归因于电子两流不稳定,预计将发生在尾迹边界区域附近。然而,这种不稳定性预计不会发生在近月尾流中(例如,约100公里的高度),因为人们认为,SW粒子的主要部分无法进入最深处的尾流,因此任何等离子体效应都将在那里不起作用。最近,日本的月球轨道飞行器“月亮女神”(SELENE)在大约100公里的高度对月球周围的等离子体和电磁环境进行了全面测量。在夜侧区域,发现了两种SW质子进入近月尾流的机制。其中之一,ii型进入,当非径向IMF成分占主导地位时变得明显,与质子的“自拾取”过程密切相关,这些质子曾经分散在月球日面表面或在磁异常周围进行磁反射。这种机制让质子进入尾流的最深处,即在SELENE轨道100公里高度的150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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Wave excitation in the lunar wake associated with solar-wind proton entry
The near-Moon space environment is characterized by formation of a plasma cavity region on the night side along the solar wind (SW) flow, which is called the lunar wake. Because the Moon obstructs the SW plasma flow, the wake region is much more tenuous than the ambient SW region. The plasma environment of the lunar wake has been considered as follows; Because high energy SW electrons can easily access the night side region while SW protons cannot, the wake region should be negatively charged. The electron-rich status of the lunar wake yields ambipolar (inward) electric field at the wake boundary where SW protons gradually come to the wake center along the interplanetary magnetic field (IMF) in the distant wake. Meanwhile, it has been reported that the SW entry into the distant wake gives rise to plasma waves. Broadband electrostatic noise (BEN) was detected by the Wind spacecraft in the distant wake (∼10,000 km from the Moon). The excitation of the BEN was attributed to ion two-stream instability owing to the SW proton beams that were accelerated/decelerated into the wake by the ambipolar electric fields. It was also attributed to electron two-stream instability that is expected to occur around the wake boundary region. However, such instabilities were not anticipated to occur in the near-Moon wake (say, ∼100 km altitude), because it has been believed that a major part of the SW particles cannot access the deepest wake so that any plasma effects would be inoperative there. Recently, a Japanese lunar orbiter SELENE (Kaguya) performed comprehensive measurements of the plasma and electromagnetic environment around the Moon at ∼100 km altitude. Concerning the night-side region, two mechanisms of SW proton entry into the near-Moon wake were found. One of them, the type-II entry, which becomes evident when the non-radial IMF component is dominant, is closely related to ‘self-pickup’ process of protons that were once scattered on the lunar dayside surface or magnetically reflected around the magnetic anomalies. This mechanism lets protons access the deepest region of the wake, namely, 150
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