论文标题
在广泛的空中阵雨中的重新恢复因子和兆元的核繁殖计算
Calculation of rescaling factors and nuclear multiplication of muons in extensive air showers
论文作者
论文摘要
从领先的宇宙射线实验获得的最新结果表明,使用LHC调节的HADRONON相互作用模型的模拟低估了与实验数据相比,广泛的空气淋浴中的MUON数量。这是所谓的妈妈赤字问题。确定空气淋浴中的muON成分对于推断主要粒子的质量至关重要,这是确定超高能量宇宙射线来源的努力的关键要素。在本文中,我们提出了一种在检测中得出muon信号的新方法,该方法使用了检测器的差异,这是使用总体构造的(数据)的主要范围(数据),但它是独立的(数据)的依赖性的,该群体是依赖于Z的范围。宇宙射线。这种方法不仅提供了测试/校准HADRONIC交互模型的机会,还提供了推导$β$指数的机会,该模型描述了淋浴中的MUON数量的增加,这是主要宇宙射线能量和质量的函数。详细的仿真显示$β$指数对望子的相互作用属性的依赖性,因此该参数的确定对于理解MUON赤字问题很重要。我们通过使用Monte Carlo模拟对EPOS-LHC和QGSJETII-04 HADRONIC相互作用模型来验证该方法,并表明该方法使我们能够在少于几个%的百分点内恢复EPOS-LHC和EPOS-LHC和QGSJETII-04和QGSJETII-04和QGSJETII-04和QGSJETII-04之间的MUON信号比率。这是分析中包括的每个主要原理的MUON信号良好恢复的结果。
Recent results obtained from leading cosmic ray experiments indicate that simulations using LHC-tuned hadronic interaction models underestimate the number of muons in extensive air showers compared to experimental data. This is the so-called muon deficit problem. Determination of the muon component in the air shower is crucial for inferring the mass of the primary particle, which is a key ingredient in the efforts to pinpoint the sources of ultra-high energy cosmic rays.In this paper, we present a new method to derive the muon signal in detectors, which uses the difference between the total reconstructed (data) and simulated signals is roughly independent of the zenith angle, but depends on the mass of the primary cosmic ray. Such a method offers an opportunity not only to test/calibrate the hadronic interaction models, but also to derive the $β$ exponent, which describes an increase of the number of muons in a shower as a function of the energy and mass of the primary cosmic ray. Detailed simulations show a dependence of the $β$ exponent on hadronic interaction properties, thus the determination of this parameter is important for understanding the muon deficit problem. We validate the method by using Monte Carlo simulations for the EPOS-LHC and QGSJetII-04 hadronic interaction models, and showing that this method allows us to recover the ratio of the muon signal between EPOS-LHC and QGSJetII-04 and the average $β$ exponent for the studied system, within less than a few percent. This is a consequence of the good recovery of the muon signal for each primary included in the analysis.