星系宇宙射线强度的各向异性及其能量依赖性的天空图

K. Munakata, N. Matsumoto, S. Yasue, C. Kato, S. Mori, M. Takita, M. Duldig, J. Humble, J. Kota
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引用次数: 3

摘要

我们分析了1985 - 2006年在日本Matsushiro (MAT)和1993 - 2005年在塔斯马尼亚Liapootah (LPT)观测到的恒星日变化。这些台站组成了位于日本和澳大利亚的地下μ子探测器的两半球网络(THN)。MAT和LPT的年平均谐波矢量基本稳定,与太阳活动周期或磁周期没有显著的相位和振幅变化。因此,本文分析了整个观测期的平均各向异性,即1985-2006年的MAT和1993-2005年的LPT。我们对THN数据采用了与Amenomori等人(2007)对西藏III数据采用的模型各向异性相同的最佳拟合分析。西藏三号实验记录的原始宇宙射线中位能量为~0.5 TeV和~5 TeV。结果表明,无论主粒子能量的数量级差异如何,最佳拟合各向异性的强度分布与西藏三号数据非常相似。这与THN观测结果一起证实了Amenomori等人(2007)基于北半球西藏三号试验的分析并没有严重偏差。另一方面,各向异性的最佳拟合幅度仅为西藏三号实验报告的三分之一或更少,表明由于太阳调制而衰减。亚tev区域各向异性振幅的刚性依赖性与Hall等(1999)报道的光谱一致,在多tev区域平滑地延伸到Tibet III结果。随着刚度的增加,高能量处的振幅几乎保持不变或逐渐减小。
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Sky-maps of the sidereal anisotropy of galactic cosmic ray intensity and its energy dependence
We analyze the sidereal daily variations observed between 1985 and 2006 at Matsushiro, Japan (MAT) and between 1993 and 2005 at Liapootah, Tasmania (LPT). These stations comprise the two hemisphere network (THN) of underground muon detectors in Japan and Australia. Yearly mean harmonic vectors at MAT and LPT are more or less stable without any significant change in phase and amplitude in correlation with either the solar activity- or magnetic-cycles. In this paper, therefore, we analyze the average anisotropy over the entire observation periods, i.e. 1985-2006 for MAT and 1993-2005 for LPT. We apply to the THN data a best-fitting analysis based on a model anisotropy in space identical to that adopted by Amenomori et al. (2007) for Tibet III data. The median energies of primary cosmic rays recorded are ~0.5 TeV for THN and ~5 TeV for the Tibet III experiment. It is shown that the intensity distribution of the best-fit anisotropy is quite similar to that derived from Tibet III data, regardless of the order of magnitude difference in energies of primary particles. This, together with the THN observations, confirms that the analysis by Amenomori et al. (2007) based on the Tibet III experiment in the northern hemisphere is not seriously biased. The best-fit amplitudes of the anisotropy, on the other hand, are only one third or less of those reported by the Tibet III experiment, indicating attenuation due to solar modulation. The rigidity dependence of the anisotropy amplitude in the sub-TeV region is consistent with the spectrum reported by Hall et al. (1999), smoothly extending to the Tibet III result in the multi-TeV region. The amplitude at higher energies appears almost constant or gradually decreasing with increasing rigidity.
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