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首页> 外文期刊>Journal of Applied Physics >Synthesis of compound thin films by dual ion beam deposition. II. Properties of aluminum‐nitrogen films
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Synthesis of compound thin films by dual ion beam deposition. II. Properties of aluminum‐nitrogen films

机译:通过双离子束沉积合成化合物薄膜。二。铝氮薄膜的性能

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We describe the properties of aluminum‐nitrogen films prepared by dual ion beam deposition in which the metal atom flux is supplied by inert ion beam sputtering and the reactive flux is supplied by a low‐energy (100–500 eV) ion beam directed at the growing film. This deposition technique and the analysis of film compositions are described in Part I of this two‐part paper.The fundamental deposition parameters of arrival rates and ion energy are controlled and directly correlated to the crystallographic structure, microstructure, and morphology of the films, over a range of composition from N/Al=0 to N/Al=1.0. Al sputter deposited in a mixture of Ar and N2 forms an expanded Al lattice with no indications of AlN formation. When the low‐energy N+2 beam is turned on, almost all the ionized nitrogen is incorporated in the film forming a mixture of large Al grains and fine grained AlN. In this two‐phase cermet region, the resistivity shows a percolation threshold at N/Al=0.45, becoming fully insulating at about N/Al=0.75. Above the arrival rate ratio N/Al=1, excess N is rejected and the films have AlN structure. For stoichiometric AlN films the texture and microstructure depend strongly on the N+2 flux and ion energy. For low ion energies (100 eV) and flux, films are formed with the c axis of the hexagonal AlN structure perpendicular to the film surface, whereas for high ion beam energies (500 eV) the c axis is close to the plane of the film. The AlN grain size also increases with nitrogen ion energy. The relative contributions of chemical driving forces and ion bombardment processes are discussed.
机译:我们描述了通过双离子束沉积制备的铝-氮薄膜的特性,其中金属原子通量通过惰性离子束溅射提供,而反应通量由低能量(100-500 eV)离子束提供,该离子束直接对准金属氮。电影。在本两部分的第一部分中介绍了这种沉积技术和膜成分的分析。控制到达速率和离子能量的基本沉积参数,并将其直接与膜的晶体结构,微观结构和形态相关。组成范围从N / Al = 0到N / Al = 1.0。溅射沉积在Ar和N2的混合物中的Al形成膨胀的Al晶格,没有迹象表明形成AlN。当打开低能N + 2束时,几乎所有离子化的氮都被掺入薄膜中,形成大的Al晶粒和细晶粒的AlN的混合物。在该两相金属陶瓷区域中,电阻率在N / Al = 0.45处显示出渗漏阈值,在大约N / Al = 0.75处变得完全绝缘。在到达速率比N / Al = 1以上,多余的N被排斥,并且膜具有AlN结构。对于化学计量的AlN薄膜,织构和微观结构在很大程度上取决于N + 2通量和离子能。对于低离子能量(100 eV)和通量,以六角AlN结构的c轴垂直于膜表面的方式形成膜,而对于高离子束能量(500 eV)的c轴则接近膜的平面。 AlN晶粒尺寸也随着氮离子能量而增加。讨论了化学驱动力和离子轰击过程的相对贡献。

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    《Journal of Applied Physics》 |1985年第1期|P.556-563|共8页
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  • 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);
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