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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Noor, N. A.
in Cooperation with on an Cooperation-Score of 37%
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Publications (3/3 displayed)
- 2024Lead free A2NaInI6 (A = Cs, Rb, K) double perovskites for optoelectronic and thermoelectric applicationscitations
- 2024Investigation of half metallic properties of Tl<sub>2</sub>Mo(Cl/Br)<sub>6</sub> double perovskites for spintronic devicescitations
- 2023Ab-initio simulations of Rb<sub>2</sub>CuMCl<sub>6</sub> (M = Sb, Bi) for photovoltaics and thermoelectric device applicationscitations
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article
Ab-initio simulations of Rb<sub>2</sub>CuMCl<sub>6</sub> (M = Sb, Bi) for photovoltaics and thermoelectric device applications
Abstract
<jats:title>Abstract</jats:title><jats:p>Due to their extraordinarily flexible optoelectronic properties, the research on non-toxic double-perovskite halides has recently become very attractive. We use density functional theory to analyze the optical, electronic, and thermoelectric characteristics of copper-based double-perovskite halides, Rb<jats:sub>2</jats:sub>CuMCl<jats:sub>6</jats:sub> (M = Sb, Bi). The band structures obtained with the Tran-Blaha altered Becke-Johnson potential demonstrate that altering the cations from Sb to Bi results in bandgap adjustments from infrared to visible (i.e. 1.0–1.2 eV) energy. Because of replacing Sb with Bi, the optical absorption exhibits utmost absorption within the ultraviolet region, whereas the absorption edge is shifted from infrared to the visible light region. Furthermore, the transport parameters are compatible with other estimated thermoelectric parameters. The fact that Rb<jats:sub>2</jats:sub>CuSbCl<jats:sub>6</jats:sub> has a higher Seebeck coefficient indicates that a narrower band gap is appropriate for thermoelectric applications compared with Rb<jats:sub>2</jats:sub>CuBiCl<jats:sub>6</jats:sub>. In general, the Rb<jats:sub>2</jats:sub>CuMCl<jats:sub>6</jats:sub> (M = Sb, Bi) is suitable for Sun-absorption devices and energy conversion, according to this computational thermoelectric and optical study.</jats:p>