The role of Anderson's rule in determining electronic, optical and transport properties of transition metal dichalcogenide heterostructuresElectronic supplementary information (ESI) available. See DOI: 10.1039/c8cp05522j

Two-dimensional (2D) transition metal dichalcogenides (TMDs) MX 2 (M = Mo, W; X = S, Se, Te) possess unique properties and novel applications in optoelectronics, valleytronics and quantum computation. In this work, we performed first-principles calculations to investigate the electronic, optical and...

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Main Authors Xu, Ke, Xu, Yuanfeng, Zhang, Hao, Peng, Bo, Shao, Hezhu, Ni, Gang, Li, Jing, Yao, Mingyuan, Lu, Hongliang, Zhu, Heyuan, Soukoulis, Costas M
Format Journal Article
LanguageEnglish
Published 12.12.2018
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Abstract Two-dimensional (2D) transition metal dichalcogenides (TMDs) MX 2 (M = Mo, W; X = S, Se, Te) possess unique properties and novel applications in optoelectronics, valleytronics and quantum computation. In this work, we performed first-principles calculations to investigate the electronic, optical and transport properties of the van der Waals (vdW) stacked MX 2 heterostructures formed by two individual MX 2 monolayers. We found that the so-called Anderson's rule can effectively classify the band structures of heterostructures into three types: straddling, staggered and broken gap. The broken gap is gapless, while the other two types possess direct (straddling, staggered) or indirect (staggered) band gaps. The indirect band gaps are formed by the relatively higher energy level of Te-d orbitals or the interlayer couplings of M or X atoms. For a large part of the formed MX 2 heterostructures, the conduction band maximum (CBM) and valence band minimum (VBM) reside in two separate monolayers, thus the electron-hole pairs are spatially separated, which may lead to bound excitons with extended lifetimes. The carrier mobilities, which depend on three competitive factors, i.e. elastic modulus, effective mass and deformation potential constant, show larger values for electrons of MX 2 heterostructures compared to their constituent monolayers. Finally, the calculated optical properties reveal strong absorption in the ultraviolet region. We have investigated the structure and electronic, mechanical, transport and optical properties of van der Waals transition metal dichalcogenide heterostructures using first-principles calculations.
AbstractList Two-dimensional (2D) transition metal dichalcogenides (TMDs) MX 2 (M = Mo, W; X = S, Se, Te) possess unique properties and novel applications in optoelectronics, valleytronics and quantum computation. In this work, we performed first-principles calculations to investigate the electronic, optical and transport properties of the van der Waals (vdW) stacked MX 2 heterostructures formed by two individual MX 2 monolayers. We found that the so-called Anderson's rule can effectively classify the band structures of heterostructures into three types: straddling, staggered and broken gap. The broken gap is gapless, while the other two types possess direct (straddling, staggered) or indirect (staggered) band gaps. The indirect band gaps are formed by the relatively higher energy level of Te-d orbitals or the interlayer couplings of M or X atoms. For a large part of the formed MX 2 heterostructures, the conduction band maximum (CBM) and valence band minimum (VBM) reside in two separate monolayers, thus the electron-hole pairs are spatially separated, which may lead to bound excitons with extended lifetimes. The carrier mobilities, which depend on three competitive factors, i.e. elastic modulus, effective mass and deformation potential constant, show larger values for electrons of MX 2 heterostructures compared to their constituent monolayers. Finally, the calculated optical properties reveal strong absorption in the ultraviolet region. We have investigated the structure and electronic, mechanical, transport and optical properties of van der Waals transition metal dichalcogenide heterostructures using first-principles calculations.
Author Ni, Gang
Zhu, Heyuan
Shao, Hezhu
Xu, Ke
Peng, Bo
Lu, Hongliang
Soukoulis, Costas M
Li, Jing
Xu, Yuanfeng
Zhang, Hao
Yao, Mingyuan
AuthorAffiliation Chinese Academy of Sciences
FORTH
Fudan University
Institute of Advanced Nanodevices
Department of Physics and Astronomy and Ames Laboratory
Institute of Electronic Structure and Laser (IESL)
Ningbo Institute of Materials Technology and Engineering
Department of Optical Science and Engineering
School of Microelectronics
Iowa State University
State Key Laboratory of ASIC and System
Key Laboratory of Micro and Nano Photonic Structures (MoE) and Key Laboratory for Information Science of Electromagnetic Waves (MoE)
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