首页> 外文期刊>Materials Chemistry and Physics >A comparison of Ar ion implantation and swift heavy Xe ion irradiation effects on immiscible AIN/TiN multilayered nanostructures
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A comparison of Ar ion implantation and swift heavy Xe ion irradiation effects on immiscible AIN/TiN multilayered nanostructures

机译:Ar离子注入和快速重Xe离子辐照对不相溶的AIN / TiN多层纳米结构的比较

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摘要

We have compared the effects of 200 keV (40)~Ar~(1+) ion implantation and 166 MeV (132)~Xe~(27+) ion irradiation on immiscible (AIN/TiN) × 5 multilayers grown on Si(l 0 0) wafers. The layers were deposited by reactive sputtering, individual layer thickness was ~22 nm (A1N) and ~32 nm (TiN), the stoichiometry A1:N ~ 45:55 and Ti:N~50:50 at%. Argon was implanted to 4 × 10~(16) ions cm~(-2), and xenon to 5 × 10~(14) ions cm~(-2). The projected Ar range is around mid depth of the multilayered structure, while swift Xe ions are buried deep into the Si substrate. Upon irradiation the structures remain essentially stable and unmixed; although in both cases we observed detectable effects. The use of wide range of irradiation parameters (S_e/S_n = 1.2-1.4, dpa = 42-63 for Ar; and S_e/S_n = 249-258, dpa = 0.03-0.05 for Xe) enabled to distinguish between the contribution of nuclear and electronic stopping. In case of Ar implantation both atomic collisions and electronic excitations contribute to the induced structural modifications, and in case of Xe only electronic excitations. It was deduced that electronic excitations generate local heating which influences lateral grain growth within individual layers, but no elemental redistribution. On the other hand, atomic collisions facilitate a low level of Ti migration into the under-stoichiometric A1N layers, in the vicinity of the implanted Ar ion range. Energy transfer and temperature distribution were evaluated and compared to the effects produced in the structures. The presented results can be interesting towards developing radiation tolerant materials.
机译:我们比较了200 keV(40)〜Ar〜(1+)离子注入和166 MeV(132)〜Xe〜(27+)离子辐照对在Si(l)上生长的不可混溶(AIN / TiN)×5多层膜的影响0 0)晶圆。通过反应溅射沉积各层,各层厚度分别为〜22 nm(AlN)和〜32 nm(TiN),化学计量比为A1:N〜45:55和Ti:N〜50:50 at%。将氩气注入到4×10〜(16)离子cm〜(-2),将氙注入到5×10〜(14)离子cm〜(-2)。预计的Ar范围在多层结构的中间深度附近,而快速的Xe离子则深埋在Si衬底中。辐照后,结构保持基本稳定且未混合;尽管在两种情况下我们都观察到了可检测的效果。使用广泛的辐照参数(对于Ar,S_e / S_n = 1.2-1.4,dpa = 42-63;对于Xe,S_e / S_n = 249-258,dpa = 0.03-0.05)能够区分核素的贡献和电子停止。在注入氩气的情况下,原子碰撞和电子激发都有助于诱导的结构改变,而在氙气的情况下,仅电子激发。可以推断出,电子激发会产生局部加热,从而影响单个层中的横向晶粒生长,但没有元素的重新分布。另一方面,原子碰撞促进了低水平的Ti迁移到注入的Ar离子范围附近的化学计量不足的AlN层中。评估能量传递和温度分布,并将其与结构中产生的效果进行比较。提出的结果对于开发耐辐射材料可能是有趣的。

著录项

  • 来源
    《Materials Chemistry and Physics》 |2012年第3期|884-892|共9页
  • 作者单位

    VINCA Institute of Nuclear Sciences, Belgrade University, P.O. Box 522, Belgrade 11001, Serbia;

    VINCA Institute of Nuclear Sciences, Belgrade University, P.O. Box 522, Belgrade 11001, Serbia;

    VINCA Institute of Nuclear Sciences, Belgrade University, P.O. Box 522, Belgrade 11001, Serbia;

    VINCA Institute of Nuclear Sciences, Belgrade University, P.O. Box 522, Belgrade 11001, Serbia;

    Jozef Stefan Institute, Jamova 39, Ljubljana 1000, Slovenia;

    Jozef Stefan Institute, Jamova 39, Ljubljana 1000, Slovenia;

    Flerov Laboratory of Nuclear Reactions, JINR, joliot-Curie St. 6, Dubna 141980, Moscow Region, Russian Federation;

    Flerov Laboratory of Nuclear Reactions, JINR, joliot-Curie St. 6, Dubna 141980, Moscow Region, Russian Federation;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    multilayers; ion implantation; irradiation effects; electron microscopy;

    机译:多层离子注入辐射效果;电子显微镜;
  • 入库时间 2022-08-18 00:39:40

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