arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2104.11277astro-ph.SR
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太阳活动24周和太阳活动极小期23/24和24/25的银河系Cosmic Ray各向异性特征

Features of the Galactic Cosmic Ray Anisotropy in the Solar Cycle 24 and Solar Minima 23/24 and 24/25

R. Modzelewska, K. Iskra, W. Wozniak, M. Siluszyk, M. V. Alania

摘要:

研究了漂移效应在银河宇宙线各向异性时间变化中的作用以及日球磁场扇形结构对银河宇宙线各向异性的影响,分析了2007-2009年第24太阳活动周和23_24太阳活动极小期以及2017- 2019年第24_25太阳活动极小期的银河宇宙线各向异性。2018年使用全球网络的数据中子。利用谐波分析方法计算了日球磁场不同扇区(正方向为正,负方向为负)的GCR各向异性的径向分量和切向分量。我们比较了GCR各向异性的分析,使用不同的评价平均GCR的刚度相关的中子监视器观测。然后用径向和切向分量来表征日球层中GCR的调制。我们发现,在2007-2009年的太阳极小期23_24,当为负值时,漂移效应在径向分量的变化中并不明显,即漂移效应被发现在2007-2009年的GCR各向异性的径向分量中产生4%的变化。因此,在2007-2009年,扩散主导的GCRs传输模型更容易接受。反过来,在2017-2018年的太阳极小期24_25附近,当为正值时,漂移效应明显可见,并在2017-2018年的GCR各向异性的径向分量中产生40%的变化。因此,在2017-2018年期间,具有明显漂移的扩散模型是可以接受的。这一结果与GCRs调制漂移理论相一致,即在负(正)极性周期中,GCRs的漂移流指向(远离)太阳,从而引起GCRs径向各向异性的22年周期变化。

英文摘要:

We study the role of drift effect in the temporal changes of the anisotropy of galactic cosmic rays (GCRs) and the influence of the sector structure of the heliospheric magnetic field on it. We analyze the GCRs anisotropy in the Solar Cycle 24 and solar minimum 23_24 with negative polarity for the period of 2007-2009 and near minimum 24_25 with positive polarity in 2017-2018 using data of global network of Neutron Monitors. We use the harmonic analyses method to calculate the radial and tangential components of the anisotropy of GCRs for different sectors (plus corresponds to the positive and minus to the negative directions) of the heliospheric magnetic field. We compare the analysis of GCRs anisotropy using different evaluations of the mean GCRs rigidity related to Neutron Monitor observations. Then the radial and tangential components are used for characterizing the GCRs modulation in the heliosphere. We show that in the solar minimum 23_24 in 2007-2009 when negative, the drift effect is not visibly evident in the changes of the radial component, i.e. the drift effect is found to produce 4 % change in the radial component of the GCRs anisotropy for 2007-2009. Hence the diffusion dominated model of GCRs transport is more acceptable in 2007-2009. In turn, near the solar minimum 24_25 in 2017-2018 when positive, the drift effect is evidently visible and produce 40% change in the radial component of the GCRs anisotropy for 2017-2018. So in the period of 2017-2018 diffusion model with noticeably manifested drift is acceptable. The results of this work are in good agreement with the drift theory of GCRs modulation, according to which during negative (positive) polarity cycles, a drift stream of GCRs is directed toward (away from) the Sun, thus giving rise to a 22-year cycle variation of the radial GCRs anisotropy.

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