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二维平面和范德瓦耳斯异质结的可控制备与光电应用

姚文乾 孙健哲 陈建毅 郭云龙 武斌 刘云圻

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二维平面和范德瓦耳斯异质结的可控制备与光电应用

姚文乾, 孙健哲, 陈建毅, 郭云龙, 武斌, 刘云圻

Controllable preparation and photoelectric applications of two-dimensional in-plane and van der Waals heterostructures

Yao Wen-Qian, Sun Jian-Zhe, Chen Jian-Yi, Guo Yun-Long, Wu Bin, Liu Yun-Qi
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  • 自石墨烯被发现以来, 二维材料因其优异的特性获得了持续且深入的探索与发展, 以石墨烯、六方氮化硼、过渡金属硫化物、黑磷等为代表的二维材料相关研究层出不穷. 随着二维新材料制备与应用探索的不断发展, 单一材料性能的不足逐渐凸显, 研究者们开始考虑采用平面拼接和层间堆垛所产生的协同效应来弥补单一材料的不足, 甚至获得一些新的性能. 利用二维材料晶格结构的匹配构建异质结, 实现特定的功能化, 或利用范德瓦耳斯力进行堆垛, 将不同二维材料排列组合, 从而在体系里引入新的自由度, 为二维材料的性质研究和实际应用打开了新的窗口. 本文从原子制造角度, 介绍了二维平面和范德瓦耳斯异质结材料的可控制备和光电应用. 首先简要介绍了应用于异质结制备的常见二维材料的分类及异质结的相关概念, 然后从原理上分类列举了常用的表征方法, 随后介绍了平面和垂直异质结的制备方法, 并对其光电性质及器件应用做了简要介绍. 最后, 对领域内存在的问题进行了讨论, 对未来发展方向做出了展望.
    Since the discovery of graphene, two-dimensional (2D) materials have received continuous attention and carried out in-depth exploration and development due to their excellent properties. With the exploration of the preparation of new 2D materials, one began to consider the synergistic effects produced by the in-plane junction and interlayer stacking to compensate for the defects of a single material and obtain some new properties. Matching the lattice structure to achieve specific functionalization, or using van der Waals force to achieve stacking, helps to introduce a new degree of freedom by combining different 2D materials, and open a new window for the research and practical application of 2D materials.From the perspective of atomic manufacturing, in this article we introduce the controllable preparation and optoelectronic applications of 2D planar and van der Waals heterojunction materials. First, we briefly introduce the common 2D materials such as graphene, hexagonal boron nitride, transition metal dichalcogenides and black phosphorus used in the preparation of heterojunctions and related concepts of heterojunctions. Second, we review, in principle, the commonly used characterization methods including scanning probe-based techniques, spectrum-based, electron-based imaging techniques and others. Third, we summarize the preparation methods of planar and vertical heterojunctions. Basically, mechanical transfer method such as wet or dry method can be used to produce various vertical heterostructures of 2D materials, but usually lack the scalability. On the other hand, chemical vapor deposition method provides a scalable route to producing the planar heterostructure and vertical structure of 2D materials. Several strategies have been developed to produce various heterostructures. In addition, the recent development of twist-angle and quasi-crystalline bi-layer graphene is briefly reviewed. Fourth, the properties and applications of 2D van der Waals heterostructures such as field-effect transistor, light emitting diode, solar cell, flexible optoelectronic devices and plasmonic applications are introduced. Finally, the problems in the field are discussed, and the outlook is provided.
      通信作者: 武斌, wubin@iccas.ac.cn ; 刘云圻, liuyq@iccas.ac.cn
    • 基金项目: 国家重点基础研究发展计划(批准号: 2016YFA0200101)、国家自然科学基金(批准号: 21633012, 61890940)、中国科学院先导B (批准号: XDB30000000)和中国科学院前沿科学重点研究计划(批准号: QYZDY-SSW-SLH029)资助的课题
      Corresponding author: Wu Bin, wubin@iccas.ac.cn ; Liu Yun-Qi, liuyq@iccas.ac.cn
    • Funds: Project supported by the National Basic Research Program of China (Grant No. 2016YFA0200101), the National Natural Science Foundation of China (Grant Nos. 21633012, 61890940), the Strategic Priority Research Program of the Chinese Academy of Sciences, China (Grant No. XDB30000000), and the CAS Key Research Program of Frontier Sciences, China (Grant No. QYZDY-SSW-SLH029)
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  • 图 1  机械转移制备vdWHs示意图 (a) 楔形转移法[43]; (b)干法转移[47]

    Fig. 1.  Schematic of mechanical transfer for the preparation of vdWHs: (a) Wedge-transfer[43]; (b) dry transfer method[47].

    图 2  h-BN沿石墨烯不同边界的外延生长 (a)刻蚀的单晶石墨烯过程示意图, 从左到右分别显示六边形单晶石墨烯、具有zigzag边界的石墨烯刻蚀孔洞、十二边形的石墨烯刻蚀图案以及具有armchair外边界图案; (b), (c) h-BN沿armchair边界生长的SEM图; (d), (e) h-BN沿zigzag和armchair边界生长的SEM图; (f) h-BN沿十二边形石墨烯边界生长的SEM图[77]

    Fig. 2.  h-BN growth along different graphene edges: (a) Schematic of different etched stages of a graphene flake showing a flake (I), etched hole with zigzag edges (II), etched dodecagonal perimeters (III), and etched perimeters with armchair edges (IV); (b), (c) SEM images of h-BN grown along armchair edges of graphene taken with different magnification; (d), (e) SEM images of h-BN stripes grown along both zigzag and armchair edges of graphene; (f) SEM image of h-BN stripes grown along edges of dodecagon graphene[77].

    图 3  MoSe2/WSe2异质结的制备 (a)以MoSe2为模板生长WSe2的示意图; (b), (c), (d)分别为MoSe2、类型I、类型II的光学显微图[75]

    Fig. 3.  The growth of MoSe2/WSe2 vdWH: (a) Diagram of MoSe2-templated WSe2 growth; (b), (c), (d) optical images of as-grown MoSe2, type I and type II[75].

    图 4  石墨烯的层层生长差异 (a), (b)铜上生长的单层定向石墨烯片SEM 图和示意图; (c), (d)铜上生长的双层石墨烯片SEM 图和示意图; (e)−(g)双层石墨烯的生长随氢气量的不同而变化[122]

    Fig. 4.  (a), (b) SEM image of aligned single layer graphene flakes grown on a solid Cu and the corresponding diagram of (a); (c), (d) SEM images of bi-layer graphene flakes grown on a solid Cu surface and the corresponding diagram of (c); (e)−(g) typical SEM images of bi-layer graphene flakes grown with H2 flow rates of 20, 35 and 50 sccm (1 sccm=1 mL/min), respectively[122].

    图 5  文章结构示意图

    Fig. 5.  Schematic diagram of materials, characterizations, synthesis, properties and applications of 2D heterostructures.

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出版历程
  • 收稿日期:  2020-08-27
  • 修回日期:  2020-09-14
  • 上网日期:  2021-01-09
  • 刊出日期:  2021-01-20

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