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使用锗探测器进行的测量以及关于宇宙μ子产生的剂量率产额的蒙特卡罗计算。

Measurements with a Ge detector and Monte Carlo computations of dose rate yields due to cosmic muons.

作者信息

Clouvas A, Xanthos S, Antonopoulos-Domis M, Silva J

机构信息

Department of Electrical and Computer Engineering, Aristotle University of Thessaloniki, GR-54006 Thessaloniki, Greece.

出版信息

Health Phys. 2003 Feb;84(2):212-21. doi: 10.1097/00004032-200302000-00009.

Abstract

The present work shows how portable Ge detectors can be useful for measurements of the dose rate due to ionizing cosmic radiation. The methodology proposed converts the cosmic radiation induced background in a Ge crystal (energy range above 3 MeV) to the absorbed dose rate due to muons, which are responsible for 75% of the cosmic radiation dose rate at sea level. The key point is to observe in the high energy range (above 20 MeV) the broad muon peak resulting from the most probable energy loss of muons in the Ge detector. An energy shift of the muon peak was observed, as expected, for increasing dimensions of three Ge crystals (10%, 20%, and 70% efficiency). Taking into account the dimensions of the three detectors the location of the three muon peaks was reproduced by Monte Carlo computations using the GEANT code. The absorbed dose rate due to muons has been measured in 50 indoor and outdoor locations at Thessaloniki, the second largest town of Greece, with a portable Ge detector and converted to the absorbed dose rate due to muons in an ICRU sphere representing the human body by using a factor derived from Monte Carlo computations. The outdoor and indoor mean muon dose rate was 25 nGy h(-1) and 17.8 nGy h(-1), respectively. The shielding factor for the 40 indoor measurements ranges from 0.5 to 0.9 with a most probable value between 0.7-0.8.

摘要

本研究表明,便携式锗探测器在测量电离宇宙辐射所致剂量率方面如何发挥作用。所提出的方法将锗晶体中由宇宙辐射诱发的本底(能量范围高于3 MeV)转换为由μ子产生的吸收剂量率,μ子在海平面宇宙辐射剂量率中占75%。关键在于在高能范围(高于20 MeV)观察锗探测器中μ子最可能的能量损失所产生的宽μ子峰。正如预期的那样,对于三种不同尺寸(效率分别为10%、20%和70%)的锗晶体,观察到了μ子峰的能量偏移。考虑到这三个探测器的尺寸,使用GEANT代码通过蒙特卡罗计算再现了三个μ子峰的位置。在希腊第二大城市塞萨洛尼基的50个室内和室外地点,使用便携式锗探测器测量了μ子产生的吸收剂量率,并通过使用从蒙特卡罗计算得出的系数,将其转换为代表人体的ICRU球体内μ子产生的吸收剂量率。室外和室内μ子平均剂量率分别为25 nGy h⁻¹和17.8 nGy h⁻¹。40次室内测量的屏蔽系数范围为0.5至0.9,最可能的值在0.7 - 0.8之间。

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