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The role of proton precipitation in the excitation of auroral FUV emissions

机译:质子沉淀在激发极光FUV排放中的作用

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摘要

Far ultraviolet remote sensing from a high-altitude satellite is extensively used to image the global aurora, derive its energetics, and follow its dynamical morphology. It is generally assumed that the observed emissions are dominated by the interaction of the precipitated electrons with the thermospheric constituents. A model to calculate far ultraviolet emissions excited by auroral electrons and protons and the secondary electrons they generate has been used to calculate the volume excitation rate of the H I Ly-alpha, O I 1304 and 1356 Å, N I 1493 Å multiplets, and the N[SUB]2[/SUB] Lyman-Birge-Hopfield (LBH) bands. The characteristic energy and the energy flux are derived from the observed statistical distribution of precipitated protons and electrons. This model is applied to the midnight aurora, the noon cusp, and a proton-dominated aurora for moderately disturbed conditions. We show that in the first two cases, direct electron impact dominates the vertically integrated emission rate over the proton component, although proton excitation plays an important role at some altitudes in the daytime cusp. In afternoon regions of the auroral zone near the auroral boundary, secondary electrons due to proton ionization are the main source of FUV emissions. The energy dependence of the efficiency of LBH band emission viewed from high altitude is calculated for electron and proton precipitations. Maps of the N[SUB]2[/SUB] LBH emission excited by both components are obtained, and regions of proton-dominated auroral emission are identified. It is found that the distribution of the ratio of proton-induced to electron-induced brightness resembles maps of the ratio of the respective precipitated energy fluxes. Proton-dominated FUV emissions are thus located in a C-shaped sector extending from prenoon to midnight magnetic local times with a maximum proton contribution near the equatorward boundary of the statistical electron oval. The distribution of the Ly-alpha/LBH intensity ratio is found to mimic the ratio of the proton flux/total energy flux, although it is insufficient by itself to accurately determine the relative fraction of auroral energy carried by the protons.
机译:远高空卫星的紫外线遥感广泛用于图像,以映像全球极光,得出其能量学,并遵循其动态形态。通常假设观察到的排放是通过沉淀电子与热散晶成分的相互作用来支配。用于计算极光电子和质子激发的远紫外线的模型以及它们产生的二次电子已经用于计算Hi Ly-α,OI 1304和1356Å,Ni1493Å倍增的体积激励率和N [ Sub] 2 [/ sub] Lyman-Birge-Hopfield(LBH)乐队。特征能量和能量通量来自观察到的沉淀质子和电子的统计分布。该模型应用于午夜极光,中午CUSP和质子主导的极光,用于适度扰乱的条件。我们表明,在前两种情况下,直接电子影响将垂直集成的排放率占Proton组件,尽管质子激发在白天令人困难的一些海拔地区发挥着重要作用。在极光边界附近的极光区的下午区域,由于质子电离导致的二级电子是FUV排放的主要来源。计算电子和质子沉淀从高海拔地区观察的LBH带发射效率的能量依赖性。获得了两种组分激发的n [sub] 2 [/ sub] lbh发射的映射,并鉴定了质子主导的极光发射区域。发现质子诱导的电子诱导亮度比的分布类似于各种沉淀能量通量的比率的图。因此,质子主导的FUV排放位于从PLENOOO延伸到午夜磁性局部时间的C形扇区,其最大质子贡献附近统计电子椭圆形的赤道边界附近。发现Ly-α/ LBH强度比的分布是模拟质子磁通/总能量通量的比例,尽管它本身不足以精确地确定由质子携带的极光能的相对分数。

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