2020 2nd Novel Intelligent and Leading Emerging Sciences Conference (NILES) 2020
DOI: 10.1109/niles50944.2020.9257929
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Optimizing SCAPS model for perovskite solar cell equivalent circuit with utilizing Matlab-based parasitic resistance estimator algorithm

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Cited by 18 publications
(8 citation statements)
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“…In order to further investigate the potential of laser-induced graphene as a counter electrode in PSC compared to gold, and to explore the impact of varying hole and electron transport layers beyond the scope of our experimental capabilities as demonstrated in section 3, we employed the SCAPS-1D simulator to analyze the J – V characteristics of different PSC configurations. In this study, we adapted our previously established SCAPS model as presented in refs , , , , and in conjunction with data sourced from the research literature. , The simulation model was initialized with the experimentally derived material parameters for TiO 2 , and NiO, serving as the electron and hole transport layers, respectively, along with FTO and LIG electrodes. Additionally, other materials were considered, such as SnO 2 as a potential electron transport layer, and copper(I) oxide (Cu 2 O) and copper bismuth thiophosphate (CBTS) for the hole transport layers, in conjunction with an Au electrode, guided by data compiled from literature sources. , …”
Section: Solar Cell Simulationmentioning
confidence: 99%
“…In order to further investigate the potential of laser-induced graphene as a counter electrode in PSC compared to gold, and to explore the impact of varying hole and electron transport layers beyond the scope of our experimental capabilities as demonstrated in section 3, we employed the SCAPS-1D simulator to analyze the J – V characteristics of different PSC configurations. In this study, we adapted our previously established SCAPS model as presented in refs , , , , and in conjunction with data sourced from the research literature. , The simulation model was initialized with the experimentally derived material parameters for TiO 2 , and NiO, serving as the electron and hole transport layers, respectively, along with FTO and LIG electrodes. Additionally, other materials were considered, such as SnO 2 as a potential electron transport layer, and copper(I) oxide (Cu 2 O) and copper bismuth thiophosphate (CBTS) for the hole transport layers, in conjunction with an Au electrode, guided by data compiled from literature sources. , …”
Section: Solar Cell Simulationmentioning
confidence: 99%
“…As a result, the J-V characteristic curve for the proposed lead-free cell was simulated as shown in Figure 6 . We used our previous perovskite solar cell modeling methodology that relies on the Solar Cell Capacitance Simulator (SCAPS-1D) program, as reported in [ 48 , 49 ]. The main theory of operation for the SCAPS-1D is based on the simulation of the electrical characteristics of solar cells, specifically their capacitance behavior.…”
Section: Low-light Energy Harvestingmentioning
confidence: 99%
“…The work functions used for contact layers are 5.1 eV for Au and 4.4 eV for FTO. The ETL and HTL defect density was stated as input parameters, while the interface defect layers, Perovskite/HTL and ETL/perovskite defect layers, were considered during the simulation procedure 24 …”
Section: Optoelectronic Modeling and Dataset Generationmentioning
confidence: 99%
“…The hole transport layer (HTL), the electron transport layer (ETL), and the electrodes are the main essentials layer constructing the PSC beside the active perovskite layer. Consequently, controlling different parameters associated with each layer can influence the overall PCE of the cell 24 . An optimum condition is targeted in such context and for each specific topology and recipe.…”
Section: Introductionmentioning
confidence: 99%
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