Abstract

<sec>Proton is the main particle component in the space radiation environment. The proton single event effect cannot be ignored with the continuous development of semiconductor technology. Accelerator simulation is the most important method to evaluate the single event effect caused by proton radiation, and the accurate measurement of proton flux is the most critical aspect in the device evaluation process. The research is based on the 100 MeV proton single-event irradiation device of the Atomic Energy Institute, which breaks through the wide-range mid-energy proton fluence rate measurement technology. The detection tools are developed such as Faraday cup, plastic scintillator detectors and secondary electron emission monitors, which can be used for measuring the proton beam current in a wide range. Faraday cup and plastic scintillator detector can be used for measuring the high flux proton and the low flux proton, respectively. Secondary electron emission monitor can be used for conducting the online real-time measurement. The proton fluxes in a range of 10<sup>6</sup>– 10<sup>7</sup> p·cm<sup>–2</sup>·s<sup>–1</sup> are measured by using two separate detectors.</sec><sec>The analysis of the fluence rate uncertainty is carried out. The uncertainty of measurement results mainly include three aspects: measurement method, measuring instrument and equipment, and repeatability of multiple measurement results. Here in this work, the Faraday cup is taken for example to analyze the uncertainty sources in the proton flux measurement. The measurement methods include the calculation of the collection efficiency of the Faraday cup (collection efficiency + escape rate = 1) and the calculation method of flux (flux = current/collection area). For the measuring instruments and equipment, mainly including 6517A and other electronic devices, their errors are determined by the accuracies of the instruments themselves. Repeatability of multiple measurement results mainly from the error caused by the instability of the accelerator beam output, the error caused by randomness of multiple measurement results, and the error given by the statistical method. The analysis shows that the uncertainty of flux measurement by Faraday cup is 7.26%, and the uncertainty of flux measurement by plastic scintillator detector is 1.64%.</sec><sec>The flux measurement of the proton fluence rate has reached the level of similar devices in the world, filling the gap in this field in China. It has a certain reference and guiding significance for the follow-up study of medium- and high-energy proton beam measurement in China. The mid-energy proton flux measurement system and uncertainty analysis method established in this study lay the foundation for accurately evaluating the component radiation effects.</sec>

Highlights

  • Range of 30 –90 MeV protons in C, Al, Fe and Cu calculated by SRIM

  • 开发了用于高注 量率质子测量的法拉第筒和低注量率质子测量的 塑料闪烁体探测器两种不同的测量方法, 突破了注 量率在 106—107 p·cm–2·s–1 之间两种探测器测量及 交叉检验, 法拉第筒和塑料闪烁体探测器测量误差 在 10% 以内, 填补了该范围注量率测量的空白

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Summary

Introduction

本文基于原子能院 100MeV 质子单粒子效应辐照装置, 突 破了宽量程中能质子注量率测量技术, 开发了法拉第筒、塑料闪烁体探测器和二次电子发射监督器等探测工 具, 可以对束流进行宽量程范围准确测量, 解决了质子注量率在 106—107 p·cm–2·s–1 范围内难以测量的关键 难题, 并进行了注量率不确定度的分析研究, 同一注量率下法拉第筒和塑料闪烁体探测器的实验测量误差与 理论分析误差相符. 质子是太空辐射环境中的主要粒子成分, 银河 宇宙射线中的质子含量为 85%, 能量分布范围从 KeV 到 GeV; 地球俘获带和太阳宇宙射线中主要 成分也是质子 [1]. 国外有关中高能质子加速器的建设及相应 的束流测量研究起步较早, 例如印第安大学回旋 加速器设施 (IUCF) 可以提供高达 205 MeV 的 质子束, 并专门设有两个质子辐照测试束线和终 端 RERS1 和 RERS2 [6], 其束流测量工具包括法拉 第筒、透射电离室、剂量胶片等. 瑞士保罗谢勒 研究所 (PSI) 和欧洲航天局 (ESA) 共同建成的质 子辐照专用装置 (PIF) 广泛应用于空间辐照以及 其他学科的研究中 [7], 其束流测量工具包括法拉 第筒、二次电子发射监督器、剂量胶片等.

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