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Improving the optical and thermoelectric properties of Cs(2)InAgCl(6) with heavy substitutional doping: a DFT insight

The next-generation indium-based lead-free halide material Cs(2)InAgCl(6) is promising for photovoltaic applications due to its good air stability and non-toxic behavior. However, its wide bandgap (>3 eV) is not suitable for the solar spectrum and hence reduces its photoelectronic efficiency for...

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Detalles Bibliográficos
Autores principales: Bhamu, K. C., Haque, Enamul, Praveen, C. S., Kumar, Nandha, Yumnam, G., Hossain, Md. Anwar, Sharma, Gautam
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8694724/
https://www.ncbi.nlm.nih.gov/pubmed/35423116
http://dx.doi.org/10.1039/d0ra01840f
Descripción
Sumario:The next-generation indium-based lead-free halide material Cs(2)InAgCl(6) is promising for photovoltaic applications due to its good air stability and non-toxic behavior. However, its wide bandgap (>3 eV) is not suitable for the solar spectrum and hence reduces its photoelectronic efficiency for device applications. Here we report a significant bandgap reduction from 2.85 eV to 0.65 eV via substitutional doping and its effects on the optoelectronic and opto-thermoelectric properties from a first-principles study. The results predict that Sn/Pb and Ga and Cu co-doping will enhance the density of states significantly near the valence band maximum (VBM) and thus reduce the bandgap via shifting the VBM upward, while alkali metals (K/Rb) slightly increase the bandgap. A strong absorption peak near the Shockley–Queisser limit is observed in the co-doped case, while in the Sn/Pb-doped case, we notice a peak in the middle of the visible region of the solar spectrum. The nature of the bandgap is indirect with Cu–Ga/Pb/Sn doping, and a significant reduction in the bandgap, from 2.85 eV to 0.65 eV, is observed in the case of Ga–Cu co-doping. We observe a significant increase in the power factor (PF) (2.03 mW m(−1) K(−2)) for the n-type carrier after Pb-doping, which is ∼3.5 times higher than in the pristine case (0.6 mW m (−1) K(−2)) at 500 K.