Band engineering of two-dimensional transition metal dichalcogenides (2D TMDCs) is of great significance with regard to both fundamental exploration and practical application. Here we report on a study of the band evolution of monolayer and bilayer TMDCs (WS2, WSe2, and MoS2) under vertical electric fields. Our results show that the electric field has a negligible influence on the bandgaps of monolayer TMDCs. For bilayer TMDCs, our results show that their intralayer direct bandgaps are also immune to the electric field. However, the indirect bandgaps of bilayer TMDCs can be effectively tuned by a vertical electric field. Interestingly, we find that the field tunability of the bandgap in bilayer WSe2 is much larger than those in bilayer WS2 and MoS2.
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19 August 2019
Research Article|
August 21 2019
Band evolution of two-dimensional transition metal dichalcogenides under electric fields
Peng Chen;
Peng Chen
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
2
State Key Laboratory for Chemo/Biosensing and Chemometrics, College of Chemistry and Chemical Engineering, Hunan University
, Changsha 410082, China
3
Department of Chemistry and Biochemistry and California Nanosystems Institute
, USA
; University of California
, Los Angeles, California 90095, USA
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
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Cai Cheng;
Cai Cheng
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
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Cheng Shen;
Cheng Shen
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
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Jing Zhang;
Jing Zhang
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
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Shuang Wu;
Shuang Wu
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
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Xiaobo Lu;
Xiaobo Lu
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
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Shuopei Wang;
Shuopei Wang
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
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Luojun Du;
Luojun Du
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
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Kenji Watanabe
;
Kenji Watanabe
5
Advanced Materials Laboratory, National Institute for Materials Science
, 1-1 Namiki, Tsukuba 305-0044, Japan
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Takashi Taniguchi;
Takashi Taniguchi
5
Advanced Materials Laboratory, National Institute for Materials Science
, 1-1 Namiki, Tsukuba 305-0044, Japan
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Jiatao Sun;
Jiatao Sun
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
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Rong Yang;
Rong Yang
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
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Dongxia Shi;
Dongxia Shi
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
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Kaihui Liu;
Kaihui Liu
6
State Key Laboratory for Mesoscopic Physics, School of Physics, Peking University
, Beijing 100871, China
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Sheng Meng;
Sheng Meng
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
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Guangyu Zhang
Guangyu Zhang
a)
1
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
4
School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100190, China
7
Collaborative Innovation Center of Quantum Matter
, Beijing 100190, China
8
Beijing Key Laboratory for Nanomaterials and Nanodevices
, Beijing 100190, China
9
Songshan-Lake Materials Laboratory
, Dongguan 523808, Guangdong Province, China
a)Author to whom correspondence should be addressed: gyzhang@iphy.ac.cn
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a)Author to whom correspondence should be addressed: gyzhang@iphy.ac.cn
Appl. Phys. Lett. 115, 083104 (2019)
Article history
Received:
February 24 2019
Accepted:
July 27 2019
Citation
Peng Chen, Cai Cheng, Cheng Shen, Jing Zhang, Shuang Wu, Xiaobo Lu, Shuopei Wang, Luojun Du, Kenji Watanabe, Takashi Taniguchi, Jiatao Sun, Rong Yang, Dongxia Shi, Kaihui Liu, Sheng Meng, Guangyu Zhang; Band evolution of two-dimensional transition metal dichalcogenides under electric fields. Appl. Phys. Lett. 19 August 2019; 115 (8): 083104. https://doi.org/10.1063/1.5093055
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