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作 者:田树平[1] 贺平逆[2] 张静全[3] 潘宇东[4] 苟富均[1]
机构地区:[1]四川大学原子核科学技术研究所,成都610064 [2]贵州大学理学院,贵阳550025 [3]四川大学材料科学与工程学院,成都610064 [4]核工业西南物理研究院,成都610041
出 处:《真空科学与技术学报》2013年第4期351-357,共7页Chinese Journal of Vacuum Science and Technology
基 金:国际热核聚变实验堆计划专项(批准号:2009GB104006);贵州省优秀青年科技人才培养计划(批准号:700968101);科技部863基金项目(合同号:2011AA050515)
摘 要:采用分子动力学方法模拟不同能量的C+离子与聚变材料钨的相互作用。模拟结果表明:当C+离子入射剂量为3.11×1016cm-2,入射能量为50 eV时,样品表面形成一层碳膜;而入射离子能量为150和250 eV时,C+离子入射到样品内与钨原子共同形成碳钨混合层,样品表面没有形成碳膜;碳的沉积率随能量的增大先减小后增加,溅射率随能量的增大先增大后减小;轰击后的样品中,碳原子密度、C-W键密度及C-C键密度分布都随能量的增加逐渐向样品内移动,且C-W键分布厚度随能量的增加而逐渐增加,C-C键分布厚度几乎不随能量变化;在作用过程中极少量的钨原子发生溅射,但引起钨晶格损伤严重;碳在轰击后的样品中主要以Csp3杂化形式存在。The interaction of the impinging C+ ion beam and the fusion material W was modeled and simulated, based on molecular dynamics, to understand the possible mechanisms responsible for the carbon deposition and carbon ion sputtering of W surface in fusion. The impacts of the interaction conditions, including the incident C+ energy and expo- sure, on the interaction were simulated. The simulated results show that the carbon atom exists mainly in sp3 state on W surfaces, and that the energy of incident C ~ strongly affects the deposition and sputtering rates. For example, as the energy increases, the deposition rate of C varies in a decrease-increase mode;whereas the sputtering rate changes in an increase- decrease mode. At an energy of 50 eV and an exposure of 3.11 ×1016 cm- 2, a thin carbon membrane forms on W sur- face,at an energy of 150 eV and 250 eV,carbon atoms are implanted in top layers of W,no carbon membrane can be ob- served. As the energy increases, the peaks of the depth profiles of C-W and C-C bonds move deeper inside W, with an in- creasingly thicker layer of C-W bond and a thickness unchanged layer of C-C bend. The sputtering of W, rarely occurs though, may seriously damage the lattice.
分 类 号:TL612[核科学技术—核技术及应用] TL627
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