McMahon C A, Fegan M F, Wong J, Long S C, Ryan T P, Colgan P A
Radiological Protection Institute of Ireland, 3 Clonskeagh Sq, Dublin 14, Ireland.
Appl Radiat Isot. 2004 Feb-Apr;60(2-4):571-7. doi: 10.1016/j.apradiso.2003.11.081.
Accurate determination of the massic activity of gamma-emitting radionuclides in environmental samples, particularly sediments and soils, cannot be achieved without taking into account sample self-absorption. The extent of self-absorption in the sample will depend on a number of factors including sample composition, density, sample size and gamma-ray energy. The preferred method for correcting for this effect is to use spiked or natural matrix reference materials that match each sample type to be analysed. However, for laboratories that must measure a wide variety of sample matrices this method is too costly and time-consuming. Another technique commonly used is to make direct gamma-ray transmission measurements for each sample. This method, while more practical, still requires a minimum of three measurements to be made for each sample analysed. A more convenient method is to prepare sets of gamma-absorption curves. This approach involves making a series of direct transmission measurements for samples of varying densities but similar type. Sets of matching samples, both spiked and unspiked, were prepared and density correction factors determined using the direct transmission method and the spiked sample approach. It was found that, for soil and sediment samples, these two methods typically differed by 5-9% for higher energy gamma rays and by 12-15% for the 59.54 keV 241Am peak. Gamma-absorption curves were also derived and, for the admittedly limited dataset, 95% confidence intervals of +/-7% for the curve generated using the spiked samples method were obtained.
如果不考虑样品的自吸收,就无法准确测定环境样品(尤其是沉积物和土壤)中发射伽马射线的放射性核素的质量活度。样品中自吸收的程度取决于许多因素,包括样品组成、密度、样品大小和伽马射线能量。校正这种效应的首选方法是使用与每种待分析样品类型相匹配的加标或天然基质参考物质。然而,对于必须测量多种样品基质的实验室来说,这种方法成本太高且耗时。另一种常用的技术是对每个样品进行直接伽马射线透射测量。这种方法虽然更实用,但对于每个分析的样品仍至少需要进行三次测量。一种更方便的方法是制备伽马吸收曲线集。这种方法包括对不同密度但类型相似的样品进行一系列直接透射测量。制备了加标和未加标的匹配样品集,并使用直接透射法和加标样品法确定了密度校正因子。结果发现,对于土壤和沉积物样品,对于较高能量的伽马射线,这两种方法通常相差5 - 9%,对于59.54 keV的241Am峰相差12 - 15%。还得出了伽马吸收曲线,对于公认有限的数据集,使用加标样品法生成的曲线获得了±7%的95%置信区间。