2021
DOI: 10.1016/j.jpcs.2021.109955
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Structural, mechanical, optoelectronic and thermoelectric properties of double perovskite compounds Cs2TeX6 (X = Br, I) for energy storage applications: First principles investigations

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Cited by 18 publications
(10 citation statements)
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“…The maximum ZT of Rb 2 PdCl 6 is 0.51 for p‐type doping at T=700 K and n=1×1021cm3 ${n=1\times {10}^{21}{cm}^{3}}$ , and the maximum ZT of Rb 2 PdBr 6 reaches up to 1.31 for p‐type at T=700 K and n=6×1020cm3 ${n=6\times {10}^{20}{cm}^{3}}$ . As we expected, the maximum ZT of Rb 2 PdBr 6 is larger than that for Rb 2 PdCl 6 , and it is also better than that for some reported vacancy‐ordered double perovskite, such as Cs 2 TiX 6 (X=Cl, Br), [10] Cs 2 TeX 6 (X=Br, I), [14] Rb 2 PtX 6 (X=Cl, Br), [15] Ga 2 PdX 6 (X=Cl, Br and I) [16] . Therefore, Rb 2 PdBr 6 is a promising p‐type thermoelectric material.…”
Section: Resultssupporting
confidence: 49%
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“…The maximum ZT of Rb 2 PdCl 6 is 0.51 for p‐type doping at T=700 K and n=1×1021cm3 ${n=1\times {10}^{21}{cm}^{3}}$ , and the maximum ZT of Rb 2 PdBr 6 reaches up to 1.31 for p‐type at T=700 K and n=6×1020cm3 ${n=6\times {10}^{20}{cm}^{3}}$ . As we expected, the maximum ZT of Rb 2 PdBr 6 is larger than that for Rb 2 PdCl 6 , and it is also better than that for some reported vacancy‐ordered double perovskite, such as Cs 2 TiX 6 (X=Cl, Br), [10] Cs 2 TeX 6 (X=Br, I), [14] Rb 2 PtX 6 (X=Cl, Br), [15] Ga 2 PdX 6 (X=Cl, Br and I) [16] . Therefore, Rb 2 PdBr 6 is a promising p‐type thermoelectric material.…”
Section: Resultssupporting
confidence: 49%
“…Among them, halide based double perovskites are suggested new type of TE materials due to good electrical transport and low phonon transport properties. Recently, thermoelectric properties of some vacancy‐ordered double perovskites have been reported, such as: Cs 2 TiX 6 (X=Cl, Br), [10] Cs 2 TeX 6 (X=Br, I), [14] Rb 2 PtX 6 (X=Cl, Br), [15] Ga 2 PdX 6 (X=Cl, Br and I) [16] . In the previously theoretical works, some approximations are adopted, including constant electron relaxation time, ignoring the lattice thermal conductivity, or ignoring phonon thermal conductivity under the Ioffe‐Regel limit [17] .…”
Section: Introductionmentioning
confidence: 99%
“…It can be observed from figure 8(c) that the value of k e /τ rises with an increase in temperature. Because of the larger ionic radii, the thermal collision increases [23].…”
Section: Thermoelectric Featuresmentioning
confidence: 99%
“…[ 22 ] First Principles calculation on Cs 2 TeX 6 (X = Br, I) were done by Bekhti Siad et al, in 2021, showed the figure of merit (ZT) of 0.71 and 0.75, respectively at room temperature. [ 23 ] The properties of K 2 NaMoX 6 (X = I, Cl) addressed by the FP‐LAPW approach and revealed that the explored compounds have ductile and anisotropic character. [ 24 ] Guechi et al [ 13 ] utilized the generalised gradient approximation (GGA) with FP‐LAPW method to examine the characteristics of Cs 2 AgBiX 6 (X = Cl, Br) materials.…”
Section: Introductionmentioning
confidence: 99%