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Extremely Low Dark Current MoS<sub>2</sub> Photodetector via 2D Halide Perovskite as the Electron Reservoir
85
Citations
37
References
2020
Year
Molybdenum DisulfideEngineeringPbi 4Halide PerovskitesOptoelectronic DevicesChemistrySemiconductorsElectronic DevicesPhotodetectorsQuantum MaterialsHigh‐performance PhotodetectorsOxide HeterostructuresElectrical EngineeringPhysicsOptoelectronic MaterialsPhotoelectric MeasurementElectron ReservoirLayered MaterialTransition Metal ChalcogenidesPerovskite Solar CellHalide PerovskiteNatural SciencesApplied PhysicsMultilayer HeterostructuresOptoelectronics
Abstract 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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