材料科学
箔法
石墨烯
扫描隧道显微镜
单层
扫描电子显微镜
低能电子衍射
单晶
结晶学
合金
基质(水族馆)
渗碳体
纳米技术
化学工程
作者
Ming Yang Huang,Mandakini Biswal,Hyo Ju Park,Sunghwan Jin,Deshun Qu,Seokmo Hong,Zhili Zhu,Lu Qiu,Da Luo,Xiaochi Liu,Zheng Yang,Zhongliu Liu,Yuan Bo Huang,Hyunseob Lim,Won Jong Yoo,Feng Ding,Yeliang Wang,Zonghoon Lee,Rodney S. Ruoff
出处
期刊:ACS Nano
[American Chemical Society]
日期:2018-05-23
卷期号:12 (6): 6117-6127
被引量:172
标识
DOI:10.1021/acsnano.8b02444
摘要
Fast-growth of single crystal monolayer graphene by CVD using methane and hydrogen has been achieved on “homemade” single crystal Cu/Ni(111) alloy foils over large area. Full coverage was achieved in 5 min or less for a particular range of composition (1.3 at.% to 8.6 at.% Ni), as compared to 60 min for a pure Cu(111) foil under identical growth conditions. These are the bulk atomic percentages of Ni, as a superstructure at the surface of these foils with stoichiometry Cu 6 Ni 1 (for 1.3 to 7.8 bulk at.% Ni in the Cu/Ni(111) foil) was discovered by low energy electron diffraction (LEED). Complete large area monolayer graphene films are either single crystal or close to single crystal, and include folded regions that are essentially parallel and that were likely wrinkles that “fell over” to bind to the surface; these folds are separated by large, wrinkle-free regions. The folds occur due to the buildup of interfacial compressive stress (and its release) during cooling of the foils from 1075 °C to room temperature. The fold heights measured by atomic force microscopy (AFM) and scanning tunneling microscopy (STM) prove them to all be 3 layers thick, and scanning electron microscopy (SEM) imaging shows them to be around 10 to 300 nm wide and separated by roughly 20 μm. These folds are always essentially perpendicular to the steps in this Cu/Ni(111) substrate. Joining of well-aligned graphene islands (in growths that were terminated prior to full film coverage) was investigated with high magnification SEM and aberration-corrected high-resolution transmission electron microscopy (TEM) as well as AFM, STM, and optical microscopy. These methods show that many of the “join regions” have folds, and these arise from interfacial adhesion mechanics (they are due to the buildup of compressive stress during cool-down, but these folds are different than for the continuous graphene films—they occur due to “weak links” in terms of the interface mechanics). Such Cu/Ni(111) alloy foils are promising substrates for the large-scale synthesis of single-crystal graphene film.
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