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Experimental determinations of beta attenuation in planar dose geometry and application to ESR dating of tooth enamel

机译:平面剂量几何中β衰减的实验测定及其在牙釉质ESR测年中的应用

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Two experiments were performed to determine the distribution of beta dose in a target medium as a function of distance from a planar source (2 pi geometry). In Experiment #1 planar absorbers were used to simulate depth in the target medium, and the attenuated dose that penetrated the intervening absorbers was detected using thermoluminescence from CaSO4:Tm. In experiment #2 pellets of powdered tooth enamel were situated in a cavity in solid tooth enamel. Dose response of the electron spin resonance (ESR) signals in the pellets allowed direct detection of dose distribution within the target medium. The dose distributions were found to agree more closely with Monte Carlo calculations and with one-group transport theory (Prestwich er al., 1997 and Brennan ct al., 1997) than with approximations used widely in ESR dating applications (Grun, 1986); Although the latter were supported by experiments by Aitken el al. (1985), the results of experiment #1 provided data to suggest that departure from 2 pi geometry was,unacceptably large in the Aitken et al. (1985) configuration. The beta doses obtained by one-group theory in typical target volumes of enamel were 17 to 40% lower than those obtained using the Grun approximation. It was concluded that one-group transport theory provides the best available routine tool for calculations of beta dose attenuation in near-planar target materials (e.g. tooth enamel and shell) irradiated by natural sources, although Monte Carlo methods are better and could eventually be introduced into-the ROSY ESR dating program (Brennan el al., 1997). It was also concluded that a revision of previously published ESR ages using one-group transport for beta dosimetry will be needed. For cases where the U concentrations in enamel are generally low (less than a few ppm), previously published ESR ages on tooth enamel are systematically too young by 5-30%. (C) 1998 Published by Elsevier Science Ltd. Air-rights reserved. [References: 10]
机译:进行了两个实验,以确定目标介质中β剂量的分布,该分布是距平面源(2 pi几何形状)的距离的函数。在实验1中,平面吸收剂用于模拟目标介质的深度,并使用来自CaSO4:Tm的热致发光检测了插入中间吸收剂的衰减剂量。在实验#2中,粉状牙釉质的小丸位于实心牙釉质的空腔中。颗粒中电子自旋共振(ESR)信号的剂量响应可直接检测目标介质中的剂量分布。剂量分布与蒙特卡洛计算和单组输运理论(Prestwich等,1997; Brennan等,1997)相比,与在ESR测年应用中广泛使用的近似值更为一致(Grun,1986)。尽管后者得到了Aitken等人的实验的支持。 (1985年),实验1的结果提供的数据表明,在Aitken等人的研究中,偏离2 pi几何尺寸的变化太大是不可接受的。 (1985)配置。通过单组理论获得的典型目标牙釉质中的β剂量比使用Grun近似获得的β剂量低17%至40%。结论是,尽管蒙特卡罗方法更好,并且最终可以引入,但单组输运理论为计算自然源辐射的近平面目标材料(例如牙釉质和贝壳)中的β剂量衰减提供了最佳的常规工具。进入ROSY ESR约会计划(Brennan等,1997)。还得出结论,将需要使用一组运输工具进行β剂量测定来修订先前公布的ESR年龄。对于牙釉质中的U浓度通常较低(小于几ppm)的情况,以前公布的牙釉质上的ESR年龄系统性地太早了5-30%。 (C)1998由Elsevier Science Ltd.发行。保留空中版权。 [参考:10]

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