Remetti Romolo, Burgio Nunzio T, Maciocco Luca, Arcese Manuele, Filannino M Azzurra
Sapienza University of Rome, Department of Energetics, via A. Scarpa 14, Rome, Italy.
Appl Radiat Isot. 2011 Jul;69(7):1046-51. doi: 10.1016/j.apradiso.2011.02.008. Epub 2011 Feb 16.
The aim of this work is quantifying the radionuclidic impurities of the irradiated [(18)O]water originated by the [(18)F]FDG synthesis process, and characterizing, from a radioprotection point of view, the waste streams produced. Two samples of 2.4ml [(18)O]H(2)O, contained in two different target cells, have been irradiated with a proton current of 37μA in a PETtrace cyclotron for about one hour each; after irradiation, without performing any chemical purification process but waiting only for the (18)F decay, they have been transferred in two vials and measured by HPGe gamma spectrometry and, subsequently, by Liquid Scintillation Counting. Previously, Monte Carlo calculations had been carried out in order to estimate the radionuclides generated within the target components ([(18)O]H(2)O, silver body and Havar® foil), with the aim to identify the nuclides expected to be found in the irradiated water. Experimental results for the two samples, normalized to the same irradiation time, show practically the same value of tritium concentration (about 36kBq/ml) while gamma emitters activity concentrations exhibit a greater spread. Considering that tritium derives from water activation while other pollutants are caused by activated cell materials released into water through erosion/corrosion mechanisms, such a spread is likely to be attributable to differences in the proton beam shape and position (production of different natural circulation patterns inside the target and different erosion mechanisms of the target cell walls). Both tritium and the other radioactive pollutants exhibit absolute values of activity and activity concentrations below the exemption limits set down in EURATOM Council Directive 96/29.
这项工作的目的是量化由[¹⁸F]FDG合成过程产生的辐照[¹⁸O]水的放射性核素杂质,并从辐射防护的角度对产生的废物流进行表征。两个分别装在不同靶盒中的2.4毫升[¹⁸O]H₂O样品,在PETtrace回旋加速器中用37μA的质子流照射约一小时;照射后,未进行任何化学纯化过程,仅等待¹⁸F衰变,然后将它们转移到两个小瓶中,先用高纯锗γ能谱法测量,随后用液体闪烁计数法测量。此前,为了估计靶组件([¹⁸O]H₂O、银体和哈瓦尔®箔)内产生的放射性核素,进行了蒙特卡罗计算,目的是确定预期在辐照水中发现的核素。两个样品的实验结果,归一化到相同的照射时间,显示氚浓度实际上具有相同的值(约36kBq/ml),而γ发射体的活度浓度则有较大差异。考虑到氚来自水的活化,而其他污染物是由通过侵蚀/腐蚀机制释放到水中的活化细胞材料引起的,这种差异可能归因于质子束形状和位置的不同(靶内不同的自然循环模式的产生以及靶盒壁的不同侵蚀机制)。氚和其他放射性污染物的活度和活度浓度绝对值均低于欧洲原子能共同体理事会指令96/29规定的豁免限值。