2018
DOI: 10.1021/acsami.7b14745
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Boosting Two-Dimensional MoS2/CsPbBr3 Photodetectors via Enhanced Light Absorbance and Interfacial Carrier Separation

Abstract: Transition metal dichalcogenides (TMDs) are promising candidates for flexible optoelectronic devices because of their special structures and excellent properties, but the low optical absorption of the ultrathin layers greatly limits the generation of photocarriers and restricts the performance. Here, we integrate all-inorganic perovskite CsPbBr nanosheets with MoS atomic layers and take the advantage of the large absorption coefficient and high quantum efficiency of the perovskites, to achieve excellent perfor… Show more

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Cited by 211 publications
(226 citation statements)
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“…As the higher laser power was directed onto the device, a higher photocurrent was generated (Figure S3, Supporting Information). We estimated the responsivity to evaluate the device performance using the following equationResponsivity R=PC / Pwhere PC is the photocurrent and P is the laser power on the channel. The responsivity decreased as the laser power increased, as shown in Figure b.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…As the higher laser power was directed onto the device, a higher photocurrent was generated (Figure S3, Supporting Information). We estimated the responsivity to evaluate the device performance using the following equationResponsivity R=PC / Pwhere PC is the photocurrent and P is the laser power on the channel. The responsivity decreased as the laser power increased, as shown in Figure b.…”
Section: Resultsmentioning
confidence: 99%
“…We calculated the external quantum efficiency (EQE) and defined the detectivity in the event that the shot noise from dark current dominated the total noise of the photodetector, as followsEQE = Rhν/e × 100%Detectivity = RA / 2eIdarkwhere A is the area of the photoactive channel, h is Planck's constant, ν is the frequency of the incident laser, and e is the unit electron charge. According to the results presented in Figure b, the highest EQE and detectivity values were 1.7 × 10 8 % and 1.9 × 10 13 Jones at the lowest power of 15 pW, respectively, as shown in Figure c.…”
Section: Resultsmentioning
confidence: 99%
“…All inorganic halide perovskite CsPbX 3 (X = I, Br, Cl) quantum dots (QDs) have recently emerged as promising candidates for optoelectronic applications such as photovoltaics, light emitters, and photodetectors, because of their tunable optical bandgap high photoluminescence with narrow emission bandwidth, attractive light absorption properties, as well as relatively high stability compared with organic–inorganic hybrid perovskite. Owing to these, considerable efforts have been devoted to breakthroughs of relative optoelectronic devices, especially the sensing devices like flexible X‐ray detectors with a sensitive detection limit of 13 nanograys s −1 and outstanding optoelectronic properties with photoresponsivity of 1.7 × 10 4 A W −1 as recently reported.…”
mentioning
confidence: 99%
“…If the compatibility issue of solution‐processed MHP nanoplatelets could be fully solved, it can significantly facilitate the processability of MHP nanoplatelets in the transistor application with probable scalable fabrication. This may also add the gate tunability to all the existing two‐terminal photodetectors and planar light‐emitting devices based on MHP nanoplatelets for enhanced device performance . As for large‐size single crystals, the main problem is how to compactly laminate the single crystal onto the transistor substrate.…”
Section: Transistors Based On Metal Halide Perovskitesmentioning
confidence: 99%