极性粒子通量分布及其空间范围

IF 4.3 3区 材料科学 Q1 ENGINEERING, ELECTRICAL & ELECTRONIC
O. Yakovchuk, Jan Maik Wissing
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引用次数: 0

摘要

背景:大气电离建模的主要挑战是使用稀疏测量来推导全球降水模式。通常,这需要对长期平均图进行密集的插值或缩放。然而,在一些区域中,粒子通量可能是相似的,这些区域的组合不会限制结果,即使它会显著提高空间和时间数据覆盖率。目的:本文的目的是统计分析被标记为极性粒子通量分布(PPFD)的地磁极附近的粒子通量分布,并确定相邻仓中的类似分布。这些仓被分组在一起,并且PPFD区域的大小被估计。好处是PPFD区域内的单个测量应该能够表示给定时间整个区域的粒子通量。方法:我们使用POES和Metop航天器在2001年至2018年期间测量的空间装仓高能粒子通量分布,来确定一个与Kp相关的区域,该区域的通量分布与在地磁极附近发现的区域相似(|magn.lat|>86°)。首先,将粒子通量绘制在磁本地时间(MLT)与磁纬度网格上。在第二步中,网格化数据根据Kp水平进行分割(形成最终的仓)。第三,每个仓中的粒子通量都经过了重新计算,以便用基于更长测量周期的速率取代零计数速率,从而使粒子分布的低通量端更加真实。然后将装仓的通量分布与PPFD进行比较。“$\Delta$测试”表示相似性。$\Delta$-测试的阈值是使用(|magn.lat|>86°)区域内$\Delta$-测试值的标准偏差定义的。结果:对于所有研究的粒子通道,都确定了极性粒子通量分布和相应的PPFD区域,电子的能量范围为154~eV-300~keV,质子的能量范围是154~eV-2.5~MeV。关于低能通道,已经确定了通量随着Kp的上升而逐渐增加。高能通道显示了背景种群和太阳粒子事件(SPE)种群的组合,它们随着Kp的增加而增加。PPFD区域的大小取决于粒子种类、能量和地磁扰动以及MLT。主要发现是:a)~存在较小但具有特征性的半球差异。b)~只有在特定能量阈值以上,PPFD区域才会随着粒子能量而增加。c)~随着Kp的升高,发现了明显的扩大——非常低的Kp除外。d)~ PPFD区域的中心向午夜移动,并随着Kp移动。边界的不对称性可以用极光强度来解释。e)~对于低能粒子,PPFD区域的主要限制似乎是极光降水。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Polar particle flux distribution and its spatial extent
Context: The main challenge in atmospheric ionisation modelling is that sparse measurements are used to derive a global precipitation pattern. Typically this requires intense interpolation or scaling of long-term average maps. In some regions however, the particle flux might be similar and a combination of these regions would not limit the results even though it would dramatically improve the spatial and temporal data coverage. Aims: The intention of this paper is to statistically analyse the particle flux distribution close to the geomagnetic poles labelled as Polar Particle Flux Distribution (PPFD) and identify similar distributions in neighbouring bins. Those bins are grouped together and the size of the PPFD-area is estimated. The benefit is that single measurements within the PPFD-area should be able to represent the particle flux for the whole area at a given time. Methods: We use spatially binned energetic particle flux distributions measured by POES and Metop spacecraft during 2001--2018 to identify a Kp-dependent area with a similar flux distribution as the one found close to the geomagnetic poles (|magn. lat|>86°). First, the particle flux is mapped on a magnetic local time (MLT) vs. magnetic latitude grid. In a second step the gridded data is split up according to Kp-levels (forming the final bins). Third, the particle flux in every bin has been recalculated in order to replace zero-count rates by rates based on longer measurement periods which results in more realistic low flux end of the particle distribution. Then the binned flux distributions are compared to the PPFD. A "$\Delta$-test" indicates the similarity. A threshold for the $\Delta$-test is defined using the standard deviation of $\Delta$-test values inside the (|magn. lat|>86°) area. Bins that meet the threshold are attributed as PPFD-area. Results: Polar Particle Flux Distributions and the corresponding PPFD-areas have been determined for all investigated particle channels, covering an energy range of 154~eV--300~keV for electrons and 154~eV--2.5~MeV for protons. Concerning low energy channels a gradual flux increase with rising Kp has been identified. High energy channels show a combination of background population and solar particle event (SPE) population that adds up with increasing Kp. The size of the PPFD-area depends on particle species, energy and geomagnetic disturbance, as well as MLT. The main findings are: a)~There are small but characteristic hemispheric differences. b)~Only above a certain energy threshold the PPFD-areas increase with particle energy. c)~A clear enlargement with rising Kp is identified - with exceptions for very low Kp. d)~The centre of the PPFD-area is shifted towards midnight and moves with Kp. Asymmetries of the boundaries could be explained by auroral intensity.   e)~For low energy particles the main restriction of the PPFD-area seems to be the auroral precipitation.
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CiteScore
7.20
自引率
4.30%
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