Murray Elanor, Zhou Ying, Slater Peter, Smith Roger, Goddard Pooja, Steele Helen
School of Chemistry, University of Birmingham, Birmingham, UK.
School of Science, Loughborough University, Loughborough, UK.
Phys Chem Chem Phys. 2022 Sep 14;24(35):20709-20720. doi: 10.1039/d2cp02244c.
This study uses molecular dynamics and barrier searching methods to investigate the diffusion and clustering of helium in plutonium dioxide. Such fundamental understanding of helium behaviour is required because radiogenic helium generated from the alpha decay of Pu nuclei can accumulate over time and storage of spent nuclear fuel needs to be safe and secure. The results show that in perfect PuO, interstitial He is not mobile over nanosecond time scales at temperatures below 1500 K with the lowest diffusion barrier being 2.4 eV. Above this temperature O vacancies can form and diffusion increases. The He diffusion barrier drops to 0.6 eV when oxygen vacancies are present. High temperature simulations show that the key He diffusion mechanism is oxygen vacancy assisted inter-site hopping rather than the direct path between adjacent interstitial sites. Unlike oxygen vacancies, plutonium vacancies act as helium traps. However, isolated substitutional He at Pu sites can be easily ejected through displacement by neighbouring interstitial Pu atoms. High temperature MD simulations show that helium can diffuse into clusters with the majority of helium clusters which form over nanosecond time scales having a He : vacancy ratio below 1 : 1. Further static calculations show that a ∼3.5 : 1 He : vacancy ratio is the largest possible for an energetically stable helium cluster. Schottky defects act as seed points for He cluster growth and a high local concentrations of He can create such defects which then pin the growing He cluster.
本研究采用分子动力学和势垒搜索方法,研究氦在二氧化钚中的扩散和聚集。由于钚核的α衰变产生的放射性氦会随时间积累,而乏核燃料的储存需要安全可靠,因此需要对氦的行为有这样的基本认识。结果表明,在完美的二氧化钚中,间隙氦在低于1500 K的温度下,在纳秒时间尺度内是不移动的,最低扩散势垒为2.4 eV。高于此温度,氧空位会形成,扩散增加。当存在氧空位时,氦的扩散势垒降至0.6 eV。高温模拟表明,氦的关键扩散机制是氧空位辅助的位点间跳跃,而不是相邻间隙位点之间的直接路径。与氧空位不同,钚空位是氦的陷阱。然而,钚位点上孤立的替代氦可以很容易地被相邻的间隙钚原子通过位移而逐出。高温分子动力学模拟表明,氦可以扩散到团簇中,在纳秒时间尺度内形成的大多数氦团簇的氦与空位比低于1:1。进一步的静态计算表明,对于能量稳定的氦团簇,最大可能的氦与空位比约为3.5:1。肖特基缺陷是氦团簇生长的种子点,高局部浓度的氦会产生这样的缺陷,进而固定生长中的氦团簇。