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Monte Carlo modelling of the propagation and annihilation of nucleosynthesis positrons in the Galaxy

机译:星系中核合成正电子的传播和and灭的蒙特卡洛模拟

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Aims. We want to estimate whether the positrons produced by the β+-decay of 26Al, 44Ti, and 56Ni synthesised in massive stars and supernovae are sufficient to explain the 511 keV annihilation emission observed in our Galaxy. Such a possibility has often been put forward in the past. In a previous study, we showed that nucleosynthesis positrons cannot explain the full annihilation emission. Here, we extend this work using an improved propagation model. Methods. We developed a Monte Carlo Galactic propagation code for ~MeV positrons in which the Galactic interstellar medium, the Galactic magnetic field, and the propagation are finely described. This code allows us to simulate the spatial distribution of the 511 keV annihilation emission. We tested several Galactic magnetic fields models and several positron escape fractions from type-Ia supernova for 56Ni positrons to account for the large uncertainties in these two parameters. We considered the collisional/ballistic transport mode and then compared the simulated 511 keV intensity spatial distributions to the INTEGRAL/SPI data. Results. Regardless of the Galactic magnetic field configuration and the escape fraction chosen for 56Ni positrons, the 511 keV intensity distributions are very similar. The main reason is that ~MeV positrons do not propagate very far away from their birth sites in our model. The direct comparison to the data does not allow us to constrain the Galactic magnetic field configuration and the escape fraction for 56Ni positrons. In any case, nucleosynthesis positrons produced in steady state cannot explain the full annihilation emission. The comparison to the data shows that (a) the annihilation emission from the Galactic disk can be accounted for; (b) the strongly peaked annihilation emission from the inner Galactic bulge can be explained by positrons annihilating in the central molecular zone, but this seems to require more positron sources than the population of massive stars and type Ia supernovae usually assumed for this region; (c) the more extended emission from the Galactic bulge cannot be explained. We show that a delayed 511 keV emission from a transient source, such as a starburst episode or a recent activity of Sgr A*, occurring between 0.3 and 10 Myr ago and producing between 1057 and 1060 sub-MeV positrons could explain this extended component, and potentially contribute to the inner bulge signal.
机译:目的我们想要估计由大质量恒星和超新星中合成的26Al,44Ti和56Ni的β+衰变产生的正电子是否足以解释我们银河系中观测到的511 keV ni灭发射。过去常常提出这种可能性。在先前的研究中,我们表明核合成正电子不能解释完整的emission灭发射。在这里,我们使用改进的传播模型扩展了这项工作。方法。我们为〜MeV正电子开发了蒙特卡洛银河传播代码,其中对银河星际介质,银河磁场和传播进行了详细描述。该代码使我们能够模拟511 keV ni灭发射的空间分布。我们针对56Ni正电子测试了一些银河磁场模型和来自Ia型超新星的若干正电子逸出分数,以说明这两个参数的巨大不确定性。我们考虑了碰撞/弹道运输模式,然后将模拟的511 keV强度空间分布与INTEGRAL / SPI数据进行了比较。结果。无论为56Ni正电子选择的银河磁场配置和逃逸分数如何,511 keV的强度分布都非常相似。主要原因是在我们的模型中〜MeV正电子不会从其出生地传播很远。与数据的直接比较不允许我们约束银河系磁场结构和56Ni正电子的逸出率。无论如何,在稳态下产生的核合成正电子不能解释完全an灭的发射。与数据的比较表明:(a)可以解释银河系盘的the灭辐射; (b)内部银河隆起的强烈ed灭辐射可以用正分子在中央分子区an没来解释,但这似乎比该地区通常假定的大质量恒星和Ia型超新星的种群需要更多的正电子源; (c)无法解释银河膨胀产生的更多辐射。我们表明,从瞬态源(例如星暴事件或Sgr A *的近期活动)发生的511 keV延迟发射发生在0.3和10 Myr之前,并产生1057和1060之间的亚MeV正电子可以解释这一扩展的成分,并可能导致内部凸起信号。

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