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核聚变与等离子体物理 ›› 2013, Vol. 33 ›› Issue (2): 127-134.

• 等离子体物理学 • 上一篇    下一篇

分子动力学模拟CH+离子与聚变材料钨的相互作用

田树平1,曹小岗1,肖家浩1,张浚源1,张静全2,潘宇东3,苟富均1   

  1. (1. 四川大学原子核科学技术研究所,成都 610064;2. 四川大学材料科学与工程学院,成都 610064;3. 核工业西南物理研究院,成都 610041)
  • 收稿日期:2012-09-04 修回日期:2013-03-04 出版日期:2013-06-15 发布日期:2013-06-14
  • 作者简介:田树平(1984-),男,四川冕宁人,硕士研究生,研究方向为等离子体与材料表面相互作用。
  • 基金资助:

    国际热核聚变实验堆(ITER)计划专项资助项目(2009GB104006);贵州省优秀青年科技人才培养计划资助项目(700968101);科技部863 基金资助项目(2011AA050515);自然科学基金支持资助课题(200010078)

Molecular dynamics simulation of interaction of ionized molecule CH+ with fusion materials-tungsten

TIAN Shu-ping1, CAO Xiao-gang1, XIAO Jia-hao1, ZHANG Jun-yuan1, ZHANG Jing-quan2,PAN Yu-dong 3, GOU Fu-jun1   

  1. (1. Institute of Nuclear Science and Technology, Key Lab of Radiation Physics & Technology Ministry of Education,Sichuan University, Chengdu 610064;2. College of Materials Science and Engineering, Sichuan University, Chengdu, 610064;3. Southwestern Institute of Physical Chengdu 610041)
  • Received:2012-09-04 Revised:2013-03-04 Online:2013-06-15 Published:2013-06-14

摘要:

采用分子动力学方法模拟了不同能量的CH+离子与聚变材料钨的相互作用。模拟结果表明:在入射过程中,能量分别为50、100 和150eV 的入射粒子,在不同入射剂量下,碳、氢原子沉积率发生突变,相互作用过程中造成少量的钨原子发生溅射,但溅射率不超过0.24%。当入射剂量达3.92×1016cm−2 左右时,入射能量为 50eV 的离子轰击样品的表面形成一层不含钨原子的碳氢薄膜,其它能量下形成钨碳氢的混合薄膜;而碳、氢原子沉积率都随入射能量的增加先减小后增加,沉积率最小值分别出现在能量为250 和200eV 时;轰击后的样品中碳氢原子、C−H、C−C、W−C 键密度分布都在向样品内移动,且样品中碳原子主要以sp3 杂化形式存在。

关键词: 电离分子动力学, 聚变材料, 沉积率, 溅射率, 钨晶格

Abstract:

The molecular dynamics simulation of interaction between CH+ with various energy and fusion material tungsten is conducted. The simulated results show that in the incident process, the sputtering rates of C and H atoms change suddenly at the different exposure doses when the incident energy is 50, 100 and 150eV respectively, a few of W atoms are sputtered in the interaction process, but the sputtering rate is less than 0.24%. When the exposure dose is about 3.92×1016cm−2, the incident energy is 50eV, a hydrocarbon firm without W atom is formed on the sample surface bombarded by the ions. A mixed film of W, C and H is formed at the other energy. The deposited rates of C and H atom first decrease then increase with the incident energy increament, the minimum deposited rats appear at 250 and 200eV respectively. The density profiles of C, H atoms, C−H, C−C, W−C bonds in the sample after bombardment move towards the inside of sample, and the C sp3 dominated the sample.

Key words: Molecular dynamics, Fusion materials, Deposited rate, Sputtering rate, W lattices

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