Co-60、Cs-137和x射线辐照源的共源TLD和RADFET表征[双极线性集成电路]

M. Simons, R. Pease, D. Fleetwood, J. Schwank, M. Krzesniak, T. Turflinger, J. Buaron, L. C. Riewe, W. Kemp, P. Duggan, A. Johnston, M.C. Wiedeman, R. Mills, A. Holmes-Siedle, L. Cohn, H. J. Doane, W.L. Lohmeier
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引用次数: 14

摘要

使用两个独立源的热释光剂量计和pMOS radfet分别测量了8个不同实验室的15个伽马源的剂量率和剂量增强(DE)因子。通过比较radfet与陶瓷和金闪光科瓦盖的反应来确定剂量增强因子。在铅/铝测试箱中测量的剂量增强因子从非常接近Co-60房间或隧道源的1.0(无增强)到封闭的Gammacell 220内的1.24不等。在Co-60房间源中,在2英寸铅砖衰减器后面的Pb/Al盒内测量了1.5至1.8之间的DE因子。Pb/Al盒内DE因子在1.17 ~ 1.3 ~ 1.4之间。从海军水面作战中心(NSWC)-Crane和桑迪亚国家实验室(SNL)的tld中确定的伽马细胞剂量率总体上接近预期水平。在ARACOR 4100 x射线源中,使用SNL双介质radfet和辐射实验与监视器(REM)厚热氧化radfet测量剂量率。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Common-source TLD and RADFET characterization of Co-60, Cs-137, and X-ray irradiation sources [bipolar linear ICs]
Dose rate and dose enhancement (DE) factors were measured at fifteen gamma sources at eight different laboratories using thermoluminescent dosimeters (TLDs) from two independent sources and pMOS RADFETs, respectively. Dose enhancement factors were determined by comparing the responses of RADFETs with ceramic and gold-flashed kovar lids. Dose enhancement factors measured within Pb/Al test enclosures varied from essentially 1.0 (no enhancement) very close to a Co-60 room or tunnel source up to 1.24 within an enclosed Gammacell 220. DE factors between 1.5 and 1.8 were measured within a Pb/Al box behind a 2-inch Pb brick attenuator in a Co-60 room source. Two Cs-137 sources evaluated were characterized by DE factors extending from 1.17 up to 1.3-1.4 inside the Pb/Al box. Gamma cell dose rates determined from TLDs from the Naval Surface Warfare Center (NSWC)-Crane and Sandia National Laboratories (SNL) were generally close to expected levels. Dose rates were measured in an ARACOR 4100 X-ray source using both SNL dual-dielectric RADFETs and Radiation Experiments and Monitors (REM) thick thermal oxide RADFETs.
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