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. 2022 Jun 21;218(5):38. doi: 10.1007/s11214-022-00885-4

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© The Author(s) 2022

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.

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Fig. 11 — (a) Location of Van Allen Probe-A (magenta), Van Allen Probe-B (blue), and Arase (black) around the time of interest. (b) Spin-averaged fluxes of ∼2.5-MeV electrons observed by Van Allen Probe-A/MagEIS (magenta), Van Allen Probe-B/MagEIS (blue), and Arase/XEP (black) as a function of $L$ -value. (c) Time after the Pc1 wave onset at ATH (0710 UT on 21 March) as a function of location of Van Allen Probe-A (magenta), Van Allen Probe-B (blue), and Arase (black) in $L$ . The $L$ -shell of this figure is the McIlwain $L$ -shell derived from Olson and Pfitzer 1977 (Olson and Pfitzer 1977) model (Kurita et al. 2018)