研究目的
Investigating the effects of solution ordered aggregation and the confinement effect of the acceptor on optimizing domain size and phase purity in all-polymer solar cells.
研究成果
The study demonstrated that promoting solution aggregation, especially the ordered structures of N2200, can effectively optimize the morphology of all-PSCs, leading to improved device performance. The blend film processed from green solvent CPME showed the smallest domain size, highest phase purity, and the best device performance.
研究不足
The study is limited to the specific polymers J51 and N2200 and the solvents chloroform, mesitylene, and cyclopentyl methyl ether. The findings may not be directly applicable to other polymer systems or solvents.
1:Experimental Design and Method Selection:
The study manipulated the domain size and phase purity of J51:N2200 blends by promoting their solution ordered aggregation and the confinement of acceptor N2200 to J51 during phase separation using three solvents (chloroform, mesitylene, and cyclopentyl methyl ether).
2:Sample Selection and Data Sources:
The polymeric donor J51 and the electron acceptor N2200 were selected for the study. The solubility of these polymers in the three solvents was tested using ultraviolet-visible (UV?vis) absorption.
3:List of Experimental Equipment and Materials:
Instruments used include UV-vis absorption spectra, photoluminescence (PL) spectra, transmission wide-angle X-ray scattering (WAXS), atomic force microscopy (AFM), transmission electron microscope (TEM), and resonant soft X-ray scattering (R-SoXS).
4:Experimental Procedures and Operational Workflow:
The study involved measuring the UV-vis spectra of J51 and N2200 in various solvents, performing WAXS characterizations, examining the surface morphology of component J51 and N2200 films via AFM, and analyzing the phase-separated morphology of blend films using TEM and R-SoXS.
5:Data Analysis Methods:
The domain sizes of the J51:N2200 blend films were calculated by an equation, ξ =2π/qmode. The relative domain purity was calculated from the scattering profiles.
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