Enhancing CsGeBr<sub>3</sub> perovskite: impact of Mn, V, and Cr doping on structural, optoelectronic, and thermoelectric properties

Abstract Perovskite materials have attracted increasing interest due to their excellent physical properties, making them particularly promising for various applications, such as optoelectronic and thermoelectric. In this paper, we investigate the effect of doping on the structural, electronic, optical, and thermoelectric properties of halogenated perovskite <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mi mathvariant="normal">CsGeBr</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>3</mml:mn> </mml:mrow> </mml:msub> </mml:math> using density functional theory (DFT). Transition metals V, Cr, and Mn introduce doping at the B site. All materials retain a stable cubic structure. Doping introduces an intermediate band related to 3d states: this is located in the conduction band for V, reaches the Fermi level for Cr, and is below it for Mn. The band gap widens with V (1.64 eV) and Cr (1.49 eV), but decreases with Mn (0.74 eV). In the latter case, the appearance of an intermediate state strongly improves the absorption in the visible ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>α</mml:mi> <mml:msub> <mml:mrow> <mml:mfenced close=")" open="(" separators=""> <mml:mrow> <mml:mi>ω</mml:mi> </mml:mrow> </mml:mfenced> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">max</mml:mi> </mml:mrow> </mml:msub> <mml:mo>=</mml:mo> <mml:mn>4.60</mml:mn> <mml:mspace width="0.25em"/> <mml:msup> <mml:mrow> <mml:mn>10</mml:mn> </mml:mrow> <mml:mn>5</mml:mn> </mml:msup> <mml:msup> <mml:mrow> <mml:mi mathvariant="normal">cm</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>1</mml:mn> </mml:mrow> </mml:msup> </mml:math> ), which makes it promising for solar cells. In parallel, Cr and V improve the thermoelectric performance, with a high-power factor and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi mathvariant="normal">ZT</mml:mi> </mml:math> figure of merit reaching 1 at 300 K in the n-type region. These modifications suggest that doping can effectively optimize the performance of perovskite-based optoelectronic and thermoelectric devices.

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Publication Details

Journal
Physica Scripta
Published
2025-05-27
DOI
https://doi.org/10.1088/1402-4896/addd71
Citations
7
Primary Topic
Perovskite Materials and Applications
Type
article
Field-Weighted Citation Impact
5.11
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article

Enhancing CsGeBr3 perovskite: impact of Mn, V, and Cr doping on structural, optoelectronic, and thermoelectric properties

F. Goumrhar, L.B. Drissi, N. El Hidaoui, R. Ahl Laamara
7 citations
Physica Scripta
Perovskite Materials and Applications
5.11
article

Enhancing CsGeBr3 perovskite: impact of Mn, V, and Cr doping on structural, optoelectronic, and thermoelectric properties

F. Goumrhar, L.B. Drissi, N. El Hidaoui, R. Ahl Laamara
article en
7 citations

Abstract

Abstract Perovskite materials have attracted increasing interest due to their excellent physical properties, making them particularly promising for various applications, such as optoelectronic and thermoelectric. In this paper, we investigate the effect of doping on the structural, electronic, optical, and thermoelectric properties of halogenated perovskite <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mrow> <mml:mi mathvariant="normal">CsGeBr</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>3</mml:mn> </mml:mrow> </mml:msub> </mml:math> using density functional theory (DFT). Transition metals V, Cr, and Mn introduce doping at the B site. All materials retain a stable cubic structure. Doping introduces an intermediate band related to 3d states: this is located in the conduction band for V, reaches the Fermi level for Cr, and is below it for Mn. The band gap widens with V (1.64 eV) and Cr (1.49 eV), but decreases with Mn (0.74 eV). In the latter case, the appearance of an intermediate state strongly improves the absorption in the visible ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>α</mml:mi> <mml:msub> <mml:mrow> <mml:mfenced close=")" open="(" separators=""> <mml:mrow> <mml:mi>ω</mml:mi> </mml:mrow> </mml:mfenced> </mml:mrow> <mml:mrow> <mml:mi mathvariant="normal">max</mml:mi> </mml:mrow> </mml:msub> <mml:mo>=</mml:mo> <mml:mn>4.60</mml:mn> <mml:mspace width="0.25em"/> <mml:msup> <mml:mrow> <mml:mn>10</mml:mn> </mml:mrow> <mml:mn>5</mml:mn> </mml:msup> <mml:msup> <mml:mrow> <mml:mi mathvariant="normal">cm</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>1</mml:mn> </mml:mrow> </mml:msup> </mml:math> ), which makes it promising for solar cells. In parallel, Cr and V improve the thermoelectric performance, with a high-power factor and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi mathvariant="normal">ZT</mml:mi> </mml:math> figure of merit reaching 1 at 300 K in the n-type region. These modifications suggest that doping can effectively optimize the performance of perovskite-based optoelectronic and thermoelectric devices.

Physica ScriptaVol. 100(7)
Mohammed V University (MA), Chouaib Doukkali University (MA), Hassan II Academy of Science and Technology (MA)
Openalex Percentile: Top 5%
Perovskite Materials and Applications
5.11
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