首页> 外文期刊>Radiochimica Acta: International Journal for Chemical Aspects of Nuclear Science and Technology >Excitation functions and yields for cyclotron production of radiorhenium via deuteron irradiation: ~(nat)W(d,xn)~*181,182(A+B),183,184(m+g),186g)Re nuclear reactions and tests on the production of ~(186g)Re using enriched ~(186)W
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Excitation functions and yields for cyclotron production of radiorhenium via deuteron irradiation: ~(nat)W(d,xn)~*181,182(A+B),183,184(m+g),186g)Re nuclear reactions and tests on the production of ~(186g)Re using enriched ~(186)W

机译:通过氘核辐射产生cyclo的回旋加速器的激发函数和产率:〜(nat)W(d,xn)〜* 181,182(A + B),183,184(m + g),186g) 〜(186g)Re使用浓缩的〜(186)W

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摘要

Excitation functions, thin- and thick-target yields for the 181-~(186g)Re and 187Wradionuclidesweremeasured by the activation stacked-foil thecnique on natural tungsten foils for deuteron energies up to 18.0MeV. These cross sections were validated by comparing the experimental results for thick-target yields with those calculated by integration of the thin-target yields. It was found that themaximum~(186g)Re content by irradiation of natural tungsten is about 55%, a higher value compared with the one found for proton beam, but not sufficient to use natural tungsten for medical purposes yet. Thus, in order to have a higher specific activity A_S of ~(186g)Re, the use of enriched ~(186)W target is necessary. Therefore the irradiation of a thick target of enriched 186Wby accelerated deuterons was studied and the results for the production of ~(186g)Re were compared with those obtained from the irradiation of the same target by accelerated protons. It was found that the deuteron irradiation is preferable for three reasons: larger yield, less contamination by tantalumradioisotopes and smaller required amount of the target, which simplify the separation of the ~(186g)Re from the target itself.
机译:通过活化叠箔技术在天然钨箔上测定氘-能量高达18.0MeV的181-(186g)Re和187W放射性核素的激发功能,薄目标厚度和厚目标产率。通过比较厚目标产量的实验结果与薄目标产量的积分计算得出的结果,验证了这些横截面。发现天然钨辐照的最大〜(186g)Re含量约为55%,比质子束中的最高,但还不足以将天然钨用于医学目的。因此,为了具有〜(186g)Re的更高的比活A_S,必须使用富集的〜(186)W靶。因此,研究了用加速氘核对富集的186W厚靶的辐照,并将〜(186g)Re的产生结果与通过加速质子辐照相同靶得到的结果进行了比较。发现氘核辐射是优选的,这有以下三个原因:产率更高,钽放射性同位素污染更少以及所需的靶标量更少,这简化了〜(186g)Re与靶标本身的分离。

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