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Extremely Low Dark Current MoS 2 Photodetector via 2D Halide Perovskite as the Electron Reservoir
Author(s) -
Wang Haoliang,
Wang Xudong,
Chen Yan,
Zhang Shukui,
Jiang Wei,
Zhang Xin,
Qin Jiajun,
Wang Jiao,
Li Xiaoguo,
Pan Yiyi,
Liu Fengcai,
Shi Zejiao,
Zhang Haijuan,
Tu Luqi,
Wang Hailu,
Long Huabao,
Li Dapeng,
Lin Tie,
Wang Jianlu,
Zhan Yiqiang,
Shen Hong,
Meng Xiangjian,
Chu Junhao
Publication year - 2020
Publication title -
advanced optical materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.89
H-Index - 91
ISSN - 2195-1071
DOI - 10.1002/adom.201901402
Subject(s) - photodetector , passivation , dark current , materials science , optoelectronics , perovskite (structure) , molybdenum disulfide , specific detectivity , halide , quenching (fluorescence) , photoluminescence , layer (electronics) , nanotechnology , optics , inorganic chemistry , chemical engineering , physics , chemistry , fluorescence , engineering , metallurgy
Toward pursuing high‐performance photodetectors based on 2D transition metal dichalcogenides (TMDs) such as molybdenum disulfide (MoS 2 ), it is desirable to reduce the high dark current and sluggish response time. Here, in multilayer MoS 2 ‐based photodetectors, a 2D halide perovskite, (C 6 H 5 C 2 H 4 NH 3 ) 2 PbI 4 ((PEA) 2 PbI 4 ), is introduced as a bifunctional material: both as electron reservoir to reduce free carriers and passivation agent to passivate defects. Surprisingly, dark current is suppressed by six orders of magnitude after coating a (PEA) 2 PbI 4 thin layer onto pristine MoS 2 photodetector, with the dark current decreased to 10 −11 A. This huge reduction of dark current suggests an efficient interlayer charge transfer from MoS 2 to (PEA) 2 PbI 4 , which is further verified by photoluminescence quenching phenomenon. It indicates that (PEA) 2 PbI 4 serves as electron reservoir to reduce carrier density of MoS 2 , resulting in ultrahigh detectivity (1.06 × 10 13 Jones). Moreover, the response speed is also accelerated by more than 100‐fold due to passivation by 2D perovskite. In addition, it is found that this type of photodetectors can further work at self‐power mode (with the bias of 0 V). Therefore, the strategy of applying 2D perovskite on the surface of TMDs provides a novel way to fabricate high‐performance photodetectors.

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