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Benchmark experiment for the cross section of the 100Mo(p,2n)99mTc and 100Mo(p,pn)99Mo reactions

机译:100Mo(p,2n)99mTc和100Mo(p,pn)99Mo反应截面的基准实验

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摘要

As nuclear medicine community has shown an increasing interest in accelerator produced 99mTc radionuclide,\udthe possible alternative direct production routes for producing 99mTc were investigated intensively.\udOne of these accelerator production routes is based on the 100Mo(p,2n)99mTc reaction. The cross section of\udthis nuclear reaction was studied by several laboratories earlier but the available data-sets are not in\udgood agreement. For large scale accelerator production of 99mTc based on the 100Mo(p,2n)99mTc reaction,\uda well-defined excitation function is required to optimise the production process effectively. One of our\udrecent publications pointed out that most of the available experimental excitation functions for the 100Mo\ud(p,2n)99mTc reaction have the same general shape while their amplitudes are different. To confirm the\udproper amplitude of the excitation function, results of three independent experiments were presented\ud(Takács et al., 2015). In this work we present results of a thick target count rate measurement of\udthe Ec = 140.5 keV gamma-line from molybdenum irradiated by Ep = 17.9 MeV proton beam, as an\udintegral benchmark experiment, to prove the cross section data reported for the 100Mo(p,2n)99mTc and\ud100Mo(p,pn)99Mo reactions in Takács et al. (2015).
机译:由于核医学界对促进剂生产的99mTc放射性核素表现出了越来越高的兴趣,\ ud深入研究了可能的替代生产途径,以生产99mTc。\ ud这些促进剂的生产途径之一是基于100Mo(p,2n)99mTc反应。这个核反应的横截面早些时候已经由几个实验室进行了研究,但是可用的数据集并不一致。对于基于100Mo(p,2n)99mTc反应的99mTc大规模加速器生产,需要明确定义的激励函数才能有效地优化生产过程。我们最近的出版物之一指出,对于100Mo \ ud(p,2n)99mTc反应,大多数可用的实验激发函数具有相同的一般形状,而它们的振幅却不同。为了确认激发函数的振幅是否合适,提出了三个独立实验的结果(Takács等,2015)。在这项工作中,我们提供了厚目标计数率测量结果的结果,即\ Ep = 17.9 MeV质子束辐照的钼的Ec = 140.5 keV伽马线,作为\ udintegral基准实验,以证明报告的横截面数据Takács等人的100Mo(p,2n)99mTc和ud100Mo(p,pn)99Mo反应。 (2015)。

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