2021
DOI: 10.1002/qua.26875
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A comprehensive computational investigations on the physical properties of TiXSb (X: Ru, Pt) half‐Heusler alloys and Ti2RuPtSb2 double half‐Heusler

Abstract: In this paper, we have investigated the structural, elastic, optoelectronic and thermoelectric properties of the new half-Heusler alloys TiXSb (X: Ru, Pt) and Ti 2 RuPtSb 2 double half-Heusler compound, using the full-potential linearized augmented plane wave method. Different approximations for the exchange-correlation functional were performed as generalized gradient approximation + Hubbard potential (GGA + U) and its combination with the modified Becke-Johnson potential. The negative values of the calculate… Show more

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Cited by 48 publications
(11 citation statements)
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“…To verify the thermodynamic stability, we calculated the formation energy of our unsynthesized EQH RuTiCrSi compound by the following expression [51]: Efgoodbreak=EtotRuTiCrSigoodbreak−)(ERubulkgoodbreak+ETibulkgoodbreak+ECrbulkgoodbreak+ESibulk$$ {E}_{\mathrm{f}}={E}_{\mathrm{tot}}^{\mathrm{Ru}\mathrm{TiCrSi}}-\left({E}_{\mathrm{Ru}}^{\mathrm{bulk}}+{E}_{\mathrm{Ti}}^{\mathrm{bulk}}+{E}_{\mathrm{Cr}}^{\mathrm{bulk}}+{E}_{\mathrm{Si}}^{\mathrm{bulk}}\right) $$ where EtotRuTiCrSi$$ {E}_{\mathrm{tot}}^{\mathrm{RuTiCrSi}} $$ is the ground‐state total energy of RuTiCrSi, ERubulk$$ {E}_{\mathrm{Ru}}^{\mathrm{bulk}} $$, ETibulk$$ {E}_{\mathrm{Ti}}^{\mathrm{bulk}} $$, ECrbulk$$ {E}_{\mathrm{Cr}}^{\mathrm{bulk}} $$, and ESibulk$$ {E}_{\mathrm{Si}}^{\mathrm{bulk}} $$ are the total energies of Ru, Ti, Cr, and Si elements in their pure bulk form, respectively. Negative formation energy (−0.27 Ry/state) indicated the theoretical stability of the EQHA RuTiCrSi.…”
Section: Resultsmentioning
confidence: 99%
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“…To verify the thermodynamic stability, we calculated the formation energy of our unsynthesized EQH RuTiCrSi compound by the following expression [51]: Efgoodbreak=EtotRuTiCrSigoodbreak−)(ERubulkgoodbreak+ETibulkgoodbreak+ECrbulkgoodbreak+ESibulk$$ {E}_{\mathrm{f}}={E}_{\mathrm{tot}}^{\mathrm{Ru}\mathrm{TiCrSi}}-\left({E}_{\mathrm{Ru}}^{\mathrm{bulk}}+{E}_{\mathrm{Ti}}^{\mathrm{bulk}}+{E}_{\mathrm{Cr}}^{\mathrm{bulk}}+{E}_{\mathrm{Si}}^{\mathrm{bulk}}\right) $$ where EtotRuTiCrSi$$ {E}_{\mathrm{tot}}^{\mathrm{RuTiCrSi}} $$ is the ground‐state total energy of RuTiCrSi, ERubulk$$ {E}_{\mathrm{Ru}}^{\mathrm{bulk}} $$, ETibulk$$ {E}_{\mathrm{Ti}}^{\mathrm{bulk}} $$, ECrbulk$$ {E}_{\mathrm{Cr}}^{\mathrm{bulk}} $$, and ESibulk$$ {E}_{\mathrm{Si}}^{\mathrm{bulk}} $$ are the total energies of Ru, Ti, Cr, and Si elements in their pure bulk form, respectively. Negative formation energy (−0.27 Ry/state) indicated the theoretical stability of the EQHA RuTiCrSi.…”
Section: Resultsmentioning
confidence: 99%
“…To verify the thermodynamic stability, we calculated the formation energy of our unsynthesized EQH RuTiCrSi compound by the following expression [51]:…”
Section: Phase Stabilitymentioning
confidence: 99%
“…We calculated the formation energy of d 0 –d HH KCrSb in the ferromagnetic state to evaluate the thermodynamic stability of our unsynthesized compound by the following expression [ 32 ] Ef=EtotKCrSb(ECrbulk+ESbbulk+EKbulk)$$E_{\text{f}} = E_{\text{tot}}^{\text{KCrSb}} - \left(\right. E_{\text{Cr}}^{\text{bulk}} + E_{\text{Sb}}^{\text{bulk}} + E_{\text{K}}^{\text{bulk}} \left.\right)$$where EtotKCrSb$E_{\text{tot}}^{\text{KCrSb}}$ is the ground‐state total energy of d 0 –d HH KCrSb, ECrbulk,ESbbulk,and EKbulk$E_{\text{Cr}}^{\text{bulk}} , E_{\text{Sb}}^{\text{bulk}} , \text{and } E_{\text{K}}^{\text{bulk}}$ are the total energies of Cr, Sb, and K elements in their pure bulk form, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…We calculated the formation energy of d 0 -d HH KCrSb in the ferromagnetic state to evaluate the thermodynamic stability of our unsynthesized compound by the following expression [32]…”
Section: Structural Properties and Phase Stabilitymentioning
confidence: 99%
“…60 The material's resistance to compressional or tensile stress in the x and y directions is related to elastic constants C 11 and C 12 , while C 44 indicates the resistance to shearing stress along a certain axis. 61 For Cs 2 TlAgF 6 , Born-Haung stability criteria is completely satisfied. 62 All mechanical characteristics are listed in Table II.…”
Section: Elastic Attributesmentioning
confidence: 97%