Electronic structure and optical properties of MAg<sub>2</sub>X<sub>3</sub> (M = Cs, K, and Rb; X = Cl, Br, and I) for potential applications as a photodetector material through DFT methods

This research demonstrates to the density functional theory (DFT) based calculations on the compounds of CsAg<sub>2</sub>I<sub>3</sub>, CsAg<sub>2</sub>Cl<sub>3</sub>, CsAg<sub>2</sub>Br<sub>3</sub>, KAg<sub>2</sub>Cl<sub>3</sub>, KAg<sub>2</sub>Br<sub>3</sub>, KAg<sub>2</sub>I<sub>3</sub>, RbAg<sub>2</sub>Cl<sub>3</sub>, RbAg<sub>2</sub>Br<sub>3</sub> and RbAg<sub>2</sub>I<sub>3</sub>. It evaluates the electronic structure, effective mass, total density of states (TDOS), partial density of states (PDOS), and optical properties of the MAg<sub>2</sub>X<sub>3</sub> (M = Cs, K, Rb; X = I, Br, Cl) compounds. The bandgap values of CsAg<sub>2</sub>I<sub>3</sub>, CsAg<sub>2</sub>Cl<sub>3</sub>, CsAg<sub>2</sub>Br<sub>3</sub>, KAg<sub>2</sub>Cl<sub>3</sub>, KAg<sub>2</sub>Br<sub>3</sub>, KAg<sub>2</sub>I<sub>3</sub>, RbAg<sub>2</sub>Cl<sub>3</sub>, RbAg<sub>2</sub>Br<sub>3</sub>, and RbAg<sub>2</sub>I<sub>3</sub> compounds have determined to be at 2.741, 2.013, 2.093, 2.097, 2.107, 2.015, 2.57, 2.133, and 2.045 eV, respectively, where CsAg2I3 2.741 eV compared experimental values (2.60 eV and 3.40 eV). The hole-effective masses for CsAg<sub>2</sub>I<sub>3</sub>, CsAg<sub>2</sub>Cl<sub>3</sub>, CsAg<sub>2</sub>Br<sub>3</sub>, KAg<sub>2</sub>Cl<sub>3</sub>, KAg<sub>2</sub>Br<sub>3</sub>, KAg<sub>2</sub>I<sub>3</sub>, RbAg<sub>2</sub>Cl<sub>3</sub>, RbAg<sub>2</sub>Br<sub>3</sub>, and RbAg<sub>2</sub>I<sub>3</sub> crystals are 0.335, 0.436, 0.197, 0.884, 0.239, 0.137, 0.765, 0.141, and 0.565, respectively. These crystals have electron effective masses of 0.788, 0.520, 0.329, 0.329, 1.024, 0.614, 0.441, 1.042, 0.490, and 1.142. The UV-visible absorption spectrum study found that CsAg<sub>2</sub>I<sub>3</sub> exhibits a steep absorption edge for 200–410nm, overlapped of 200–400nm of reference. Moreover, elastic constant, complex dielectric function, absorption coefficient, direct band energy, indirect band energy, and Urbach energy have been studied. The outcomes are auspicious for a future high-performance Ag halide perovskite-based photodetector material.

Publication Details

Journal
Figshare
Published
2025-01-01
DOI
https://doi.org/10.6084/m9.figshare.29364146.v1
Primary Topic
Heusler alloys: electronic and magnetic properties
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article
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article

Electronic structure and optical properties of MAg2X3 (M = Cs, K, and Rb; X = Cl, Br, and I) for potential applications as a photodetector material through DFT methods

Figshare
Heusler alloys: electronic and magnetic properties
article

Electronic structure and optical properties of MAg2X3 (M = Cs, K, and Rb; X = Cl, Br, and I) for potential applications as a photodetector material through DFT methods

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Abstract

This research demonstrates to the density functional theory (DFT) based calculations on the compounds of CsAg<sub>2</sub>I<sub>3</sub>, CsAg<sub>2</sub>Cl<sub>3</sub>, CsAg<sub>2</sub>Br<sub>3</sub>, KAg<sub>2</sub>Cl<sub>3</sub>, KAg<sub>2</sub>Br<sub>3</sub>, KAg<sub>2</sub>I<sub>3</sub>, RbAg<sub>2</sub>Cl<sub>3</sub>, RbAg<sub>2</sub>Br<sub>3</sub> and RbAg<sub>2</sub>I<sub>3</sub>. It evaluates the electronic structure, effective mass, total density of states (TDOS), partial density of states (PDOS), and optical properties of the MAg<sub>2</sub>X<sub>3</sub> (M = Cs, K, Rb; X = I, Br, Cl) compounds. The bandgap values of CsAg<sub>2</sub>I<sub>3</sub>, CsAg<sub>2</sub>Cl<sub>3</sub>, CsAg<sub>2</sub>Br<sub>3</sub>, KAg<sub>2</sub>Cl<sub>3</sub>, KAg<sub>2</sub>Br<sub>3</sub>, KAg<sub>2</sub>I<sub>3</sub>, RbAg<sub>2</sub>Cl<sub>3</sub>, RbAg<sub>2</sub>Br<sub>3</sub>, and RbAg<sub>2</sub>I<sub>3</sub> compounds have determined to be at 2.741, 2.013, 2.093, 2.097, 2.107, 2.015, 2.57, 2.133, and 2.045 eV, respectively, where CsAg2I3 2.741 eV compared experimental values (2.60 eV and 3.40 eV). The hole-effective masses for CsAg<sub>2</sub>I<sub>3</sub>, CsAg<sub>2</sub>Cl<sub>3</sub>, CsAg<sub>2</sub>Br<sub>3</sub>, KAg<sub>2</sub>Cl<sub>3</sub>, KAg<sub>2</sub>Br<sub>3</sub>, KAg<sub>2</sub>I<sub>3</sub>, RbAg<sub>2</sub>Cl<sub>3</sub>, RbAg<sub>2</sub>Br<sub>3</sub>, and RbAg<sub>2</sub>I<sub>3</sub> crystals are 0.335, 0.436, 0.197, 0.884, 0.239, 0.137, 0.765, 0.141, and 0.565, respectively. These crystals have electron effective masses of 0.788, 0.520, 0.329, 0.329, 1.024, 0.614, 0.441, 1.042, 0.490, and 1.142. The UV-visible absorption spectrum study found that CsAg<sub>2</sub>I<sub>3</sub> exhibits a steep absorption edge for 200–410nm, overlapped of 200–400nm of reference. Moreover, elastic constant, complex dielectric function, absorption coefficient, direct band energy, indirect band energy, and Urbach energy have been studied. The outcomes are auspicious for a future high-performance Ag halide perovskite-based photodetector material.

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Heusler alloys: electronic and magnetic properties
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