Cosmic Gamma-Ray Spectroscopy

R. Diehl
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引用次数: 10

Abstract

Abstract Penetrating gamma-rays require complex instrumentation for astronomical spectroscopy measurements of gamma-rays from cosmic sources. Multiple-interaction detectors in space combined with sophisticated post-processing of detector events on ground have lead to a spectroscopy performance which is now capable to provide new astrophysical insights. Spectral signatures in the MeV regime originate from transitions in the nuclei of atoms (rather than in their electron shell). Nuclear transitions are stimulated by either radioactive decays or high-energy nuclear collisions such as with cosmic rays. Gamma-ray lines have been detected from radioactive isotopes produced in nuclear burning inside stars and supernovae, and from energetic-particle interactions in solar flares. Radioactive-decay gamma-rays from 56Ni directly reflect the source of supernova light. 44Ti is produced in core-collapse supernova interiors, and the paucity of corresponding 44Ti gamma-ray line sources reflects the variety of dynamical conditions herein. 26 Al and 60Fe are dispersed in interstellar space from massive-star nucleosynthesis over millions of years. Gamma-rays from their decay are measured in detail by gamma-ray telescopes, astrophysical interpretations reach from massive-star interiors to dynamical processes in the interstellar medium. Nuclear de-excitation gamma-ray lines have been found in solar-flare events, and convey information about energetic-particle production in these events, and their interaction in the solar atmosphere. The annihilation of positrons leads to another type of cosmic gamma-ray source. The characteristic annihilation gamma-rays at 511 keV have been measured long ago in solar flares, and now throughout the interstellar medium of our Milky Way galaxy. But now a puzzle has appeared , as a surprising predominance of the central bulge region was determined. This requires either new positron sources or transport processes not yet known to us. In this paper we discuss instrumentation and data processing for cosmic gamma-ray spectroscopy, and the astrophysical issues and insights from these measurements.
宇宙伽马射线光谱学
穿透伽玛射线需要复杂的天文光谱仪器来测量来自宇宙源的伽玛射线。空间中的多重相互作用探测器与地面探测器事件的复杂后处理相结合,导致了光谱性能,现在能够提供新的天体物理见解。MeV状态下的光谱特征来自原子核的跃迁(而不是它们的电子壳层)。核跃迁是由放射性衰变或高能核碰撞(如与宇宙射线的碰撞)激发的。从恒星和超新星内部核燃烧产生的放射性同位素,以及太阳耀斑中的能量粒子相互作用中,已经探测到伽马射线线。来自56Ni的放射性衰变伽马射线直接反射超新星的光源。44Ti是在核心坍缩超新星内部产生的,对应的44Ti伽玛射线线源的稀少反映了其中动态条件的多样性。数百万年来,Al和60Fe在大质量恒星核合成过程中分散在星际空间中。它们衰变产生的伽马射线通过伽马射线望远镜进行了详细测量,天体物理学解释从大质量恒星内部到星际介质中的动态过程。在太阳耀斑事件中发现了核去激发伽马射线线,并传达了这些事件中能量粒子产生的信息,以及它们在太阳大气中的相互作用。正电子的湮灭导致了另一种类型的宇宙伽马射线源。511kev的特征湮灭伽马射线很久以前就在太阳耀斑中被测量到,现在在我们银河系的星际介质中也被测量到。但现在一个谜出现了,因为中央凸起区域的优势被确定为惊人的。这要么需要新的正电子源,要么需要我们还不知道的传输过程。在本文中,我们讨论了宇宙伽马射线光谱学的仪器和数据处理,以及这些测量的天体物理问题和见解。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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