论文标题
在太阳磁场逆转期间,宇宙射线的展开漂移效果
Unfolding Drift Effects for Cosmic Rays over the Period of the Sun's Magnetic Field Reversal
论文作者
论文摘要
采用一个完善的,全面的3-D数值调节模型来模拟2011年5月至2015年5月的银河质子,电子和正气子,包括太阳能周期的太阳能磁性逆转24的逆转。目的是评估这些模拟与1.0-3.0 GV的相对方法相比,这些模拟与该方法相比的相比,以下方面的方法是如何进行的。尤其是粒子漂移,从负到正磁极循环。除了局部星际光谱,电子和正电子仅在漂移模式方面有所不同,但是它们在质子方面有所不同,例如其他方式,例如其绝热能量在较低的刚性下变化。为了完成对相对电荷颗粒的模拟,也获得了抗蛋白酶建模结果。共同的观测和相应的建模表明在最近的极性逆转之前和之后的漂移模式差异,并在很大程度上澄清了在此期间电荷符号依赖性现象。在没有明确定义的磁性极性的这一时期,全球颗粒漂移的效果变得可忽略不计。在极性逆转期间,所有颗粒的MFP的低值在太阳最小活动期间对比其大值,因此暴露了不同调制过程的相对贡献和影响,从太阳能最小值到最大活性。我们发现,在极性逆转之后,漂移量表开始恢复,但是MFP在极性反转后的一段时间内不断减小或保持不变。
A well-established, comprehensive 3-D numerical modulation model is applied to simulate galactic protons, electrons and positrons from May 2011 to May 2015, including the solar magnetic polarity reversal of Solar Cycle 24. The objective is to evaluate how these simulations compare with corresponding AMS observations for 1.0-3.0 GV, and what underlying physics follows from this comparison in order to improve our understanding on how the major physical modulation processes change, especially particle drift, from a negative to a positive magnetic polarity cycle. Apart from their local interstellar spectra, electrons and positrons differ only in their drift patterns, but they differ with protons in other ways such as their adiabatic energy changes at lower rigidity. In order to complete the simulations for oppositely charged particles, antiproton modeling results are obtained as well. Together, the observations and the corresponding modeling indicate the difference in the drift pattern before and after the recent polarity reversal and clarify to a large extent the phenomenon of charge-sign dependence during this period. The effect of global particle drift became negligible during this period of no well-defined magnetic polarity. The resulting low values of all particles' MFPs during the polarity reversal contrast their large values during solar minimum activity, and as such expose the relative contributions and effects of the different modulation processes from solar minimum to maximum activity. We find that the drift scale starts recovering just after the polarity reversal, but the MFPs keep decreasing or remain unchanged for some period after the polarity reversal.