研究目的
To synthesize CH3NH3PbX3 (X = Cl, Br, I) perovskite quantum dots at room temperature in the open air using short-chain C4H9NH3X (X = Cl, Br, I) as the unique capping agent and to improve the morphology of CH3NH3PbBr3 thin films.
研究成果
The short-chain C4H9NH3X (X = Cl, Br, I) can be used to synthesize CH3NH3PbX3 (X = Cl, Br, I) perovskite quantum dots at room temperature in air and improve the morphology of MAPbBr3 thin films, which will benefit the fabrication of high-performance light-emitting diodes.
研究不足
The pure MAPbI3 QDs are more sensitive to the air, making it difficult to obtain pure MAPbI3 QDs solution in ambient conditions via this approach. The alloyed MAPbX3 (X=Br, I) QDs have relative wide FWHMs and low PLQYs due to the unstability of MAPbI3 QDs in air.
1:Experimental Design and Method Selection:
The synthesis of CH3NH3PbX3 perovskite quantum dots was conducted at room temperature in the open air using short-chain C4H9NH3X as the capping agent. The morphology of CH3NH3PbBr3 thin films was improved by spin-coating a solution of CH3NH3Br, C4H9NH3Br, and PbBr2 in N, N-dimerthylformamide.
2:Sample Selection and Data Sources:
Materials used include PbCl2, PbBr2, PbI2, methylamine, butylamine, HCl, HBr, HI, N, N-dimerthylformamide, dimethylsulfoxide, and toluene.
3:List of Experimental Equipment and Materials:
UV-vis absorption spectra were recorded by Metash 5200 spectrophotometer. Photoluminescence spectra were measured using Shimadzu RF 5301PC. The relative photoluminescence quantum yields were obtained by comparing the integrated emission of the QD samples with a standard fluorescence dye.
4:Experimental Procedures and Operational Workflow:
The synthesis process involved dissolving CH3NH3Br and PbBr2 in DMF, adding C4H9NH3Br, and then dropping the precursor solution into toluene under vigorous stirring to form quantum dots. Thin films were fabricated by spin-coating the precursor solution on soda lime glass substrates followed by sintering at 90°C in air.
5:Data Analysis Methods:
The luminescence decay curve was programmed from a Lecroy Wave Runner 6100 digital oscilloscope using a tunable laser as the excitation source. The temperature dependent PL spectra were collected by a Maya 2000 Pro CCD-based fiber optic spectrometer.
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Shimadzu RF 5301PC
RF 5301PC
Shimadzu
Measuring photoluminescence spectra
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Lecroy Wave Runner 6100 digital oscilloscope
Wave Runner 6100
Lecroy
Programming the luminescence decay curve
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Bruker D8 FOCUS X-ray diffractometer
D8 FOCUS
Bruker
Monitoring XRD patterns
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FEI Tecnai G2 F20
Tecnai G2 F20
FEI
Obtaining HR-TEM images
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Hitachi S-4800
S-4800
Hitachi
Taking SEM images
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Metash 5200 spectrophotometer
5200
Metash
Recording UV-vis absorption spectra
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Maya 2000 Pro CCD-based fiber optic spectrometer
Maya 2000 Pro
Ocean Optics Inc.
Collecting temperature dependent PL spectra
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ET9000
ET9000
East Changing Technologies Inc.
Measuring the carrier mobility of thin films
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Bruker AXS XFlash detector 4010
XFlash detector 4010
Bruker AXS
Recording EDS
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