4.5 Article

Fabrication, characterization and simulation analysis of perovskite solar cells with dopant-free solution-processible C6PcH2 hole transporting material

期刊

OPTICAL AND QUANTUM ELECTRONICS
卷 54, 期 5, 页码 -

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SPRINGER
DOI: 10.1007/s11082-022-03638-3

关键词

Fabrication; Perovskite; Solar cells; Characterization; Phthalocyanine

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A new design of perovskite solar cells (PSCs) with non-peripherally substituted octahexylphthalocyanine (C6PcH(2)) hole transporting material (HTM) and MoOx buffer layer was introduced. Experiment and simulation analysis were conducted to evaluate the photovoltaic performance of the PSCs based on C6PcH(2) HTMs. The results showed that the PSCs exhibited good performance and simulation analysis suggested potential improvements at lower temperatures.
A new design of perovskite solar cells (PSCs) with non-peripherally substituted octahexylphthalocyanine (C6PcH(2)) hole transporting material (HTM) and MoOx buffer layer was introduced through experiment and simulation analysis. The external quantum efficiency (EQE) and current density-voltage (JV) characteristics were performed to analyze the photovoltaic performance of the PSCs based on C6PcH(2) HTMs. The EQE was over 73% within the visible region (at 450 nm) but lower at 740 nm due to parasitic light absorption of C6PcH(2) molecules. As a result, a short-circuit current density (J(sc)) J(sc) = 16.3 mA/cm(2), open-circuit voltage (V-oc) V-oc = 0.95 V, fill factor (FF) FF = 35%, and a power conversion efficiency PCE = 5.4% were recorded under reverse bias scans (from open-circuit to short-circuit). Simulation analysis with Silvaco and SCAPS-1D was also performed to support the carrier transport analysis of PSCs with C6PcH(2) HTM as well their photovoltaic performance in temperature range from 303 to 258 K, in which the charge carrier mobility of C6PcH(2) molecules were strongly improved. By reducing the temperature from 303 to 258 K, the simulated PCE of 19.6% was achieved for the PSCs utilizing C6PcH(2) as an HTM. The difference in PCEs between the synthesized and simulated devices was in part due to the alignment of C6PcH(2) molecules in thin film. The simulation results closely supported the experiment and promised an improved performance upon realizing unknown electro-optical semiconductor properties of the C6PcH(2) layer.

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