2019
DOI: 10.1002/inf2.12031
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Metal halide perovskite nanocrystals and their applications in optoelectronic devices

Abstract: In recent years, metal halide perovskite nanocrystals (NCs) have been favored by many researchers due to their unique properties including long carrier diffusion length, high carrier mobility, tunable emission wavelength, and narrow full width at half maximum, making them great application potentials in optoelectronic devices. The photoluminescence quantum yields of perovskite NCs are nearly 100%, and the device efficiency of perovskite NC‐based light‐emitting diodes (LEDs) has been improved significantly from… Show more

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Cited by 79 publications
(55 citation statements)
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“…Integration of various photodetectors with different light‐sensitive materials and detecting capacity is an inevitable way to achieve the color/spectrum detection. However, the ingredient photodetector was usually individually prepared with uneven performance in most of the previous works 17,18. The existence of the cask effect would drag the overall performance behind, especially the response speed.…”
Section: Figurementioning
confidence: 99%
“…Integration of various photodetectors with different light‐sensitive materials and detecting capacity is an inevitable way to achieve the color/spectrum detection. However, the ingredient photodetector was usually individually prepared with uneven performance in most of the previous works 17,18. The existence of the cask effect would drag the overall performance behind, especially the response speed.…”
Section: Figurementioning
confidence: 99%
“…A perovskite light absorber with an ideal bandgap and crystallization quality is the first hurdle of an artificial photon energy harvesting system 24. For perovskite materials with a crystal structure of ABX 3 , the composition engineering of A‐site and X‐site elements is an effective way to tune the bandgap 25–29.…”
Section: Resultsmentioning
confidence: 99%
“…To predict the 3D structure forming possibility, Goldschmidt tolerance factor ( t ) and octahedral factor ( μ ) are used as empirical rules. The definitions of t and μ are as following: t=RA+RX2()RB+RX, μ=RnormalBRnormalX where R A , R B , and R X are the effective radii of the A, B, and X ions, respectively . For a well‐established 3D network, t and μ are usually in the range of 0.8‐1.0 and 0.44‐0.9, respectively .…”
Section: Introductionmentioning
confidence: 99%
“…, and R X are the effective radii of the A, B, and X ions, respectively. 31,32 For a well-established 3D network, t and μ are usually in the range of 0.8-1.0 and 0.44-0.9, respectively. 10 Non-perovskite structures are often observed for impropersized ions, for example, large A cations like CH 3 CH 2 NH 3 + (t > 1.0) and small A cations like Rubidium (t < 0.8) will both lead to the collapse of the 3D structured network.…”
Section: Introductionmentioning
confidence: 99%