Structural stabilities, robust half-metallicity, magnetic anisotropy, and thermoelectric performance of the pristine/Ir-doped Sr<sub>2</sub>CaOsO<sub>6</sub>: strain modulations

Half-metallic (HM) ferromagnetic (FM)/ferrimagnetic (FIM) materials with a large energy-gap (<i>E</i> <sub>g</sub>) and high magnetocrystalline anisotropy energy (MAE) are receiving consideration for their potential usage in solid-state electronic devices. This study explores various traits of the pristine (prs.)/Ir-doped (dop.) Sr<sub>2</sub>CaOsO<sub>6</sub> structure using <i>ab initio</i> calculations, where Ir is doped at the Os-site. To determine the synthesis feasibility of the structures under ambient conditions, the formation energy, elastic constants, and phonon curves are determined. The prs. structure manifests a FM semiconducting nature with an <i>E</i> <sub>g</sub> of 0.048 eV. Strikingly, the Ir-dop. structure becomes HM FIM because additional electrons provided by the dopant (Ir) cause a repulsion in the Os t<sup>2</sup> <sub>2g</sub> spin-minority channel, resulting in conductivity. Conversely, an <i>E</i> <sub>g</sub> of 1.15 eV in the spin-majority channel exists, which is high enough to keep the HM state stable. The computed partial spin-moment on the Os in the prs. system is 1.19 <i>μ</i> <sub>B</sub>. In the Ir-dop. system it is 1.09/-1.39 <i>μ</i> <sub>B</sub> on the Os/Ir ion holding an Os<sup>+6</sup>/Ir<sup>+4</sup> state with electronic distributions of 5d<sup>2</sup>(t<sup>2</sup> <sub>2g</sub>↑t<sup>0</sup> <sub>2g</sub>↓e<sup>0</sup> <sub>g</sub>↑e<sup>0</sup> <sub>g</sub>)/5d<sup>5</sup>(t<sup>3</sup> <sub>2g</sub>↑t<sup>2</sup> <sub>2g</sub>↓e<sup>0</sup> <sub>g</sub>↑e<sup>0</sup> <sub>g</sub>) with . Further, the spin-magnetization density isosurfaces assist in determining the <i>m</i> <sub>s</sub> values and FM/FIM state of the prs./Ir-dop. system holding a Curie temperature (<i>T</i> <sub>C</sub>) of 185/171 K. Besides this, we computed the thermoelectric properties of the prs./Ir-dop. motifs; the figure of merit (0.33/0.02), Seebeck coefficient (147/30 μV K<sup>-1</sup>), and low thermal conductivity (0.21/0.71 × 10<sup>19</sup> Ωm<sup>-1</sup> s<sup>-1</sup>) at 300 K highlight their potential for conversion devices. Interestingly, a semiconducting-to-HM transition is predicted at a crucial compressive strain of -3% in the prs. structure. Conversely, the HM state in the dop. structure displays robustness against strain. Additionally, it is shown that an applied tensile strain can significantly improve <i>ZT</i>, while compressive strains illustrate a positive impact on the <i>T</i> <sub>C</sub> value.

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Publication Details

Journal
RSC Advances
Published
2025-01-01
DOI
https://doi.org/10.1039/d5ra02453f
Citations
3
Primary Topic
Advanced Condensed Matter Physics
Type
article
Field-Weighted Citation Impact
3.77

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article

Structural stabilities, robust half-metallicity, magnetic anisotropy, and thermoelectric performance of the pristine/Ir-doped Sr2CaOsO6: strain modulations

Safdar Nazir, Saira Shahzadi, Ihab Mohamed Moussa, Sohail Mumtaz
3 citations
RSC Advances
Advanced Condensed Matter Physics
3.77
article

Structural stabilities, robust half-metallicity, magnetic anisotropy, and thermoelectric performance of the pristine/Ir-doped Sr2CaOsO6: strain modulations

Safdar Nazir, Saira Shahzadi, Ihab Mohamed Moussa, Sohail Mumtaz
article en
3 citations

Abstract

Half-metallic (HM) ferromagnetic (FM)/ferrimagnetic (FIM) materials with a large energy-gap (<i>E</i> <sub>g</sub>) and high magnetocrystalline anisotropy energy (MAE) are receiving consideration for their potential usage in solid-state electronic devices. This study explores various traits of the pristine (prs.)/Ir-doped (dop.) Sr<sub>2</sub>CaOsO<sub>6</sub> structure using <i>ab initio</i> calculations, where Ir is doped at the Os-site. To determine the synthesis feasibility of the structures under ambient conditions, the formation energy, elastic constants, and phonon curves are determined. The prs. structure manifests a FM semiconducting nature with an <i>E</i> <sub>g</sub> of 0.048 eV. Strikingly, the Ir-dop. structure becomes HM FIM because additional electrons provided by the dopant (Ir) cause a repulsion in the Os t<sup>2</sup> <sub>2g</sub> spin-minority channel, resulting in conductivity. Conversely, an <i>E</i> <sub>g</sub> of 1.15 eV in the spin-majority channel exists, which is high enough to keep the HM state stable. The computed partial spin-moment on the Os in the prs. system is 1.19 <i>μ</i> <sub>B</sub>. In the Ir-dop. system it is 1.09/-1.39 <i>μ</i> <sub>B</sub> on the Os/Ir ion holding an Os<sup>+6</sup>/Ir<sup>+4</sup> state with electronic distributions of 5d<sup>2</sup>(t<sup>2</sup> <sub>2g</sub>↑t<sup>0</sup> <sub>2g</sub>↓e<sup>0</sup> <sub>g</sub>↑e<sup>0</sup> <sub>g</sub>)/5d<sup>5</sup>(t<sup>3</sup> <sub>2g</sub>↑t<sup>2</sup> <sub>2g</sub>↓e<sup>0</sup> <sub>g</sub>↑e<sup>0</sup> <sub>g</sub>) with . Further, the spin-magnetization density isosurfaces assist in determining the <i>m</i> <sub>s</sub> values and FM/FIM state of the prs./Ir-dop. system holding a Curie temperature (<i>T</i> <sub>C</sub>) of 185/171 K. Besides this, we computed the thermoelectric properties of the prs./Ir-dop. motifs; the figure of merit (0.33/0.02), Seebeck coefficient (147/30 μV K<sup>-1</sup>), and low thermal conductivity (0.21/0.71 × 10<sup>19</sup> Ωm<sup>-1</sup> s<sup>-1</sup>) at 300 K highlight their potential for conversion devices. Interestingly, a semiconducting-to-HM transition is predicted at a crucial compressive strain of -3% in the prs. structure. Conversely, the HM state in the dop. structure displays robustness against strain. Additionally, it is shown that an applied tensile strain can significantly improve <i>ZT</i>, while compressive strains illustrate a positive impact on the <i>T</i> <sub>C</sub> value.

RSC AdvancesVol. 15(22)
Gachon University (KR), University of Sargodha (PK), King Saud University (SA)
King Saud University, Taif University
Openalex Percentile: Top 7%
Advanced Condensed Matter Physics
3.77
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