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Etude de l'oxydation thermique du titane et du zirconium sous irradiation aux ions d'argon dans le domaine du MeV (E ≤ 15 MeV)

机译:MeV域(E≤15 MeV)中氩离子辐照下钛和锆的热氧化研究

摘要

We have shown that argon ion irradiation between 1 and 15 MeV produces damage on both titanium and zirconium surfaces, taking the form of accelerated oxidation and/or craterization effects, varying as a function of the projectile energy and the annealing atmosphere (temperature and pressure) simulating the environmental conditions of the fuel/cladding interface of PWR fuel rods. Using AFM, we have shown that the titanium and zirconium surface is attacked under light argon ion bombardment at high temperature (up to 500°C) in weakly oxidizing medium (under rarefied dry air pressure ranging from 5,7 10-5 Pa to 5 10-3 Pa) for a fixed fluence of about 5 1014 ions.cm-2. We observed the formation of nanometric craters over the whole titanium surface irradiated between 2 and 9 MeV and the whole zirconium surface irradiated at 4 MeV, the characteristics of which vary depending on the temperature and the pressure. In the case of the Ar/Ti couple, the superficial damage efficiency increases when the projectile energy decreases from 9 to 2 MeV. Moreover, whereas the titanium surface seems to be transparent under the 15-MeV ion beam, the zirconium surface exhibits numerous micrometric craters surrounded by a wide halo. The crater characteristics (size and superficial density) differ significantly from that observed both in the low energy range (keV) where the energy losses are controlled by ballistic collisions (Sn) and in the high energy range (MeV - GeV) where the energy losses are controlled by electronic excitations (Se), which was not completely unexpected in this intermediate energy range for which combined Sn - Se stopping power effects are possibly foreseen. Using XPS associated to ionic sputtering, we have shown that there is an irradiation effect on thermal oxidation of titanium, enhanced under the argon ion beam between 2 and 9 MeV, and that there is also an energy effect on the oxide thickness and stoichiometry. The study conducted using Spectroscopic Ellipsometry on the oxide films grown between 1 and 9 MeV confirmed these results and showed precisely that there is an oxidation peak as a function of the argon ion energy, found maximum at 3 MeV under present experimental conditions. The oxygen gain measurements obtained by NBS confirm the presence of this oxidation peak. Until now, the results obtained by NBS concerning the thermal oxidation of zirconium under argon irradiation at 4 and 9 MeV confirm the previous works done by the 'Aval du Cycle Electronucléaire' group of the 'Institut de Physique Nucléaire de Lyon', and strongly suggest the existence of the oxidation peak in the same projectile energy range, as for titanium.
机译:我们已经表明,在1到15 MeV之间的氩离子辐照会以加速的氧化和/或弹坑效应的形式在钛和锆表面上产生损伤,其随弹丸能量和退火气氛(温度和压力)的变化而变化。模拟压水堆燃料棒燃料/包层界面的环境条件。使用原子力显微镜(AFM),我们已经表明,钛和锆的表面在弱氧化介质中(在稀有的干燥空气压力为5.7 10-5 Pa至5的高温下)于高温(最高500°C)下受到轻氩离子轰击而受到腐蚀。 10-3 Pa)的固定通量约为5 1014 ions.cm-2。我们观察到在2到9 MeV之间辐照的整个钛表面和在4 MeV下辐照的整个锆表面上都形成了纳米坑,其特性随温度和压力而变化。在Ar / Ti对的情况下,当射弹能量从9 MeV降低到2 MeV时,表面损伤效率增加。此外,尽管钛表面在15 MeV离子束的作用下似乎是透明的,但锆表面却显示出许多被宽广的光环包围的微米级缩孔。弹坑特性(尺寸和表观密度)与在低能量范围(keV)(能量损失由弹道碰撞(Sn)控制)和高能量范围(MeV-GeV)(能量损失受能量损失控制)明显不同通过电子激发(Se)来控制,这在这个中间能量范围内并不是完全出乎意料的,对于该中间能量范围,可以预见到Sn-Se组合的停止功率效应。使用与离子溅射相关的XPS,我们已经表明,在2到9 MeV的氩离子束下,钛对钛的热氧化有辐照作用,并且在氧化物厚度和化学计量上也有能量效应。使用光谱椭偏仪对生长在1到9 MeV之间的氧化膜进行的研究证实了这些结果,并精确地表明,存在一个作为氩离子能量的函数的氧化峰,在当前实验条件下,该峰出现在3 MeV处。通过NBS获得的氧气增益测量结果证实了该氧化峰的存在。迄今为止,国家统计局关于在4 MeV和9 MeV的氩气照射下锆热氧化的结果证实了“里昂物理核研究所”的“ Aval du CycleElectronucléaire”小组所做的先前工作,并强烈建议在与钛相同的射弹能量范围内,存在氧化峰。

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    Do Ngoc-Long;

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  • 年度 2012
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