关于为什么10-TeV宇宙射线碰撞起源于本地星际介质

M. Malkov, Patrick H. Diamond, Mingyun Cao, Igor Moskalenko
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引用次数: 1

摘要

最近对主要和次要CR光谱的测量,它们的到达方向,以及我们对日球层周围磁场几何形状的改进,使我们能够设定一个距离界限,超过这个界限,令人费解的10-TeV“碰撞”就不可能产生。与碰撞相关的光谱断裂的锐度,CR强度在局部磁赤道上的突变($90^{\circ}$俯仰角),以及主CR和次CR光谱模式之间的相似性表明碰撞粒子在背景CR之外的局部重新加速。我们认为,附近的冲击可以通过将先前存在的CRs的刚度增加约1.5倍来产生这样的颠簸。低于~0.5 TV的再加速粒子与星际介质流对流,无法到达太阳,因此产生了碰撞。这一单一的普遍过程是导致在100 TV以下刚性范围内观察到的所有CR物种光谱的原因。我们提出一个可行的候选者是与距太阳3.2%的Epsilon Eridani星相关的激波系统,它与当地磁场的方向很好地对齐。其他的冲击,比如古老的超新星壳,可能会产生类似的效果。我们提供了一个简单的公式,可以再现所有CR物质的光谱,只有三个参数是唯一从CR质子数据中得到的。我们展示了我们的形式如何预测氦和碳光谱以及B/C比。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
On Why the 10-TeV Cosmic Ray Bump Originates in the Local Interstellar Medium
Recent measurements of primary and secondary CR spectra, their arrival directions, and our improved knowledge of the magnetic field geometry around the heliosphere allow us to set a bound on the distance beyond which a puzzling 10-TeV"bump"cannot originate. The sharpness of the spectral breaks associated with the bump, the abrupt change of the CR intensity across the local magnetic equator ($90^{\circ}$ pitch angle), and the similarity between the primary and secondary CR spectral patterns point to a local reacceleration of the bump particles out of the background CRs. We argue that a nearby shock may generate such a bump by increasing the rigidity of the preexisting CRs below 50 TV by a mere factor of ~1.5. Reaccelerated particles below ~0.5 TV are convected with the interstellar medium flow and do not reach the Sun, thus creating the bump. This single universal process is responsible for the observed spectra of all CR species in the rigidity range below 100 TV. We propose that one viable candidate is the system of shocks associated with Epsilon Eridani star at 3.2 pc of the Sun, which is well aligned with the direction of the local magnetic field. Other shocks, such as old supernova shells, may produce a similar effect. We provide a simple formula that reproduces the spectra of all CR species with only three parameters uniquely derived from the CR proton data. We show how our formalism predicts helium and carbon spectra and the B/C ratio.
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