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使用康普顿成像光谱仪对聚甲基丙烯酸甲酯体模的伽马射线散射进行成像

Imaging of Gamma-ray Scatter from a Polymethyl-methacrylate Phantom Using a Compton Imaging Spectrometer.

作者信息

Frank Samuel J, Kearfott Kimberlee J

机构信息

*University of Michigan, Department of Nuclear Engineering and Radiological Sciences, Ann Arbor, MI 48109-2104.

出版信息

Health Phys. 2017 Aug;113(2):135-142. doi: 10.1097/HP.0000000000000681.

Abstract

Commercially available gamma-ray imaging spectrometers have been introduced recently and are currently undergoing investigations for various applications in nuclear power plants, environmental management, and medical environments. A Compton imaging gamma-ray spectrometer uses an array of detectors or a single position-sensitive crystal to create planar images of radionuclide distributions. The typical software included with these devices creates images of specific radionuclides using only the counts under their known gamma emission photopeaks. This approach prevents the direct imaging of scattered radiation, which is of interest for many radiation protection applications. In this paper, a technique for imaging radiation scatter or portions of the scatter spectrum is implemented. This involves the creation of a virtual radionuclide in software with peaks placed throughout the backscatter continuum of interest and then imaging that virtual radionuclide in the post-processing software. This technique is used to image the Compton scatter successfully from a polymethyl-methacrylate (PMMA) phantom placed in a Cs irradiator beam. Measured scatter energies were found to be within 15% of the expected values, sufficient to predict scatter behavior and individually measure separate sources of scatter at different angles.

摘要

市售的伽马射线成像光谱仪最近已被推出,目前正在核电站、环境管理和医疗环境等各种应用中接受研究。康普顿成像伽马射线光谱仪使用探测器阵列或单个位置敏感晶体来创建放射性核素分布的平面图像。这些设备随附的典型软件仅使用已知伽马发射光峰下的计数来创建特定放射性核素的图像。这种方法无法对散射辐射进行直接成像,而散射辐射在许多辐射防护应用中是令人感兴趣的。在本文中,实现了一种对辐射散射或散射光谱部分进行成像的技术。这涉及在软件中创建一个虚拟放射性核素,其峰放置在整个感兴趣的反向散射连续谱中,然后在后处理软件中对该虚拟放射性核素进行成像。该技术成功用于对放置在铯辐照束中的聚甲基丙烯酸甲酯(PMMA)模型的康普顿散射进行成像。发现测量的散射能量在预期值的15%以内,足以预测散射行为并单独测量不同角度下的散射源。

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