2017 IEEE International Conference on Smart Grid and Smart Cities (ICSGSC) 2017
DOI: 10.1109/icsgsc.2017.8038549
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Numerical analysis of czts solar cell with in2s3 buffer layer: a study of a czts based thin film solar cell, concerning the effects of several parameters on its electrical performance

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Cited by 4 publications
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“…Chemical bath deposition was used to create Cu S bS 2 thin films on a glass substrate. It is a highly doped p‐type material, also, it is an alternative absorber layer material used as a BSF layer in the present work because of its earth‐abundance, low cost, and non‐toxic nature 17,22–25 . Here, In 2 Se 3 and Ag 2 S have been deliberately selected as buffer layers to explore their morphology and structure to accurately represent the results of simulations; CuSbS 2 is taken as the BSF layer.…”
Section: Introductionmentioning
confidence: 99%
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“…Chemical bath deposition was used to create Cu S bS 2 thin films on a glass substrate. It is a highly doped p‐type material, also, it is an alternative absorber layer material used as a BSF layer in the present work because of its earth‐abundance, low cost, and non‐toxic nature 17,22–25 . Here, In 2 Se 3 and Ag 2 S have been deliberately selected as buffer layers to explore their morphology and structure to accurately represent the results of simulations; CuSbS 2 is taken as the BSF layer.…”
Section: Introductionmentioning
confidence: 99%
“…It is a highly doped p-type material, also, it is an alternative absorber layer material used as a BSF layer in the present work because of its earth-abundance, low cost, and non-toxic nature. 17,[22][23][24][25] Here, In 2 Se 3 and Ag 2 S have been deliberately selected as buffer layers to explore their morphology and structure to accurately represent the results of simulations; CuSbS 2 is taken as the BSF layer. Basic electronic and optical properties of CuSbS 2 material include an almost ideal direct band gap of 1.37 eV to 1.58 eV and greater broad-spectrum optical absorption (10 5 cm À1 ), a moderate acceptor concentration (10 16 -10 20 cm À3 ), chemically stable phase, and a low melting point (551 C), appear to be approaching p-type material for PV cells.…”
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confidence: 99%
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“…A research investigation successfully attained an efficiency of 18.66% with a 2000 nm thick CZTS absorber layer and a 100 nm thick CdS buffer layer [10]. Additionally, a different approach obtained 18.68% efficiency by employing FTO as the window layer, In 2 S 3 as the buffer layer, CZTS as the absorber layer and Mo as back contact [11], while another study on CZTS SC recorded 19.23% efficiency with a ZnO window layer, a 50 nm thick In 2 S 3 buffer layer, and a 1000 nm thick CZTS absorber layer [12]. A photovoltaic device composed of the Al-ZnO/CdS/CZTS/MoO 3 /Au structure achieved a PCE of 22.28% during an in-vestigation into the utilization of MoO 3 as the back-surface field.…”
Section: Introductionmentioning
confidence: 99%