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Interface and interaction of graphene layers on SiC(000(1)over-bar) covered with TiC(111) intercalation

机译:石墨烯层对具有TIC(111)插入的SiC(000(1)覆盖条)上的界面和相互作用

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摘要

It is important to understand the interface and interaction between the graphene layer, titanium carbide [TiC(111)] interlayer, and silicon carbide [SiC(000 (1) over bar)] substrates in epitaxial growth of graphene on silicon carbide (SiC) substrates. In this study, the fully relaxed interfaces which consist of up to three layers of TiC(111) coatings on the SiC(000 (1) over bar) as well as the graphene layers interactions with these TiC(111)/SiC(000 (1) over bar) were systematically studied using the density functional theory-D2 (DFT-D2) method. The results showed that the two layers of TiC(111) coating with the C/C-terminated interfaces were thermodynamically more favorable than one or three layers of TiC(111) on the SiC(000 (1) over bar). Furthermore, the bonding of the Ti-hollow-site stacked interfaces would be a stronger link than that of the Ti-Fccsite stacked interfaces. However, the formation of the C/Ti/C and Ti/C interfaces implied that the first upper carbon layer can be formed on TiC(111)/SiC(000 (1) over bar) using the decomposition of the weaker Ti-C and C-Si interfacial bonds. When growing graphene layers on these TiC(111)/SiC(000 (1) over bar) substrates, the results showed that the interaction energy depended not only on the thickness of the TiC(111) interlayer, but also on the number of graphene layers. Bilayer graphene on the two layer thick TiC(111)/SiC(000 (1) over bar) was thermodynamically more favorable than a monolayer or trilayer graphene on these TiC(111)/ SiC(000 (1) over bar) substrates. The adsorption energies of the bottom graphene layers with the TiC(111)/SiC(000 (1) over bar) substrates increased with the decrease of the interface vertical distance. The interaction energies between the bottom, second and third layers of graphene on the TiC(111)/SiC(000 (1) over bar) were significantly higher than that of the freestanding graphene layers. All of these findings provided insight into the growth of epitaxial graphene on TiC(111)/SiC(000 (1) over bar) substrates and the design of graphene/TiC/SiC-based electronic devices.
机译:理解所述石墨烯层之间的界面和相互作用是很重要的,碳化钛[的TiC(111)]中间层和碳化硅[SiC(下000(1)在巴)]在对碳化硅的石墨烯的外延生长的衬底(SiC)的基板。在这项研究中,完全松弛接口,其由最多的TiC的三个层在SiC(000(1)在巴)(111)的涂层的以及与这些的TiC(111)/ SiC(下000的石墨烯层的相互作用( 1)在巴)使用密度泛函理论-D2(DFT-D2)的方法进行了系统研究。结果表明,具有C / C封端界面的两层TiC(111)涂层在SiC(000(1)上方的SiC(000(1)上)热力学上比一个或三层TiC(111)更有利。此外,Ti-中空部位堆叠接口的键合将是比Ti-FcCsite堆叠界面更强的链路。然而,C / TI / C和TI / C接口的形成暗示,使用弱TI-C的分解,可以在TIC(111)/ SiC(000(1)上)形成第一上碳层和c-si界面键。当在这些TIC(111)/ SiC(000(1)上)基板上生长石墨烯层时,结果表明,相互作用能量不仅依赖于TIC(111)中间层的厚度,而且还依赖于石墨烯的数量层。两层厚TiC(111)/ SiC(000(1)上方的双层石墨烯在这些TiC(111)/ SiC(000(1)上方)基板上的单层或三层石墨烯进行热力学依赖。底部石墨烯层的吸附能量与TIC(111)/ SiC(000(1)上方)基板随界面垂直距离的降低而增加。在TiC(111)/ siC(000(1)上方的石墨烯上的底部,第二和第三层之间的相互作用能显着高于独立的石墨烯层。所有这些发现都提供了对TIC(111)/ SiC(000(1)上的外延石墨烯的生长的洞察,以及石墨烯/ TiC / SiC的电子设备的设计。

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  • 作者单位

    Nanjing Tech Univ Sch Chem &

    Mol Engn IAS Nanjing 211816 Jiangsu Peoples R China;

    Nanjing Tech Univ Sch Chem &

    Mol Engn IAS Nanjing 211816 Jiangsu Peoples R China;

    Nanjing Tech Univ Sch Chem &

    Mol Engn IAS Nanjing 211816 Jiangsu Peoples R China;

    Harbin Inst Technol Dept Phys Harbin 150001 Heilongjiang Peoples R China;

    Shantou Univ Dept Chem Shantou 515063 Guangdong Peoples R China;

    Nanjing Tech Univ Sch Chem &

    Mol Engn IAS Nanjing 211816 Jiangsu Peoples R China;

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  • 正文语种 eng
  • 中图分类 物理学;化学;
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