2020
DOI: 10.1016/j.jmrt.2020.06.086
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Physical characteristics of CdZrO3 perovskite at different pressure for optoelectronic application

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Cited by 33 publications
(13 citation statements)
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“…The peaks are noted at trueB 2.6 eV (3.7), trueD3.91 eV (7.9) for Rb 2 PdCl 6 and trueA 2.1 eV (2.9), trueC 3.7 eV (6.5) Rb 2 PdBr 6 the values are overestimated in small and depressed as compared to ε 2 ( ω ) due to density functional used here. Furthermore, external doping and pressure has been used in cubic systems 49‐51 to tune electronic and optical properties, same strategy would be effective in the studied materials as well.…”
Section: Resultsmentioning
confidence: 99%
“…The peaks are noted at trueB 2.6 eV (3.7), trueD3.91 eV (7.9) for Rb 2 PdCl 6 and trueA 2.1 eV (2.9), trueC 3.7 eV (6.5) Rb 2 PdBr 6 the values are overestimated in small and depressed as compared to ε 2 ( ω ) due to density functional used here. Furthermore, external doping and pressure has been used in cubic systems 49‐51 to tune electronic and optical properties, same strategy would be effective in the studied materials as well.…”
Section: Resultsmentioning
confidence: 99%
“…At 0eV, both NaRaF 3 and RbRaF 3 have conductivity values of 0 (real and imaginary). The most important optical property is the energy loss function which describes the energy ability to conduct and loss of energy [ [54] , [55] , [56] , [57] ]. The major peak of the loss function for NaRaF 3 is 21.016eV, while for RbRaF 3 it is 21.150eV where the maximum energy will be a loss.…”
Section: Resultsmentioning
confidence: 99%
“…Therefore, the ultralow values of κ l which are consistent with Cs 2 PtI 6 (0.17 W/mK), 15 and the potential of studied materials for thermoelectric applications. Since external pressure and element doping are widely used strategies to tune electronic properties of cubic systems, 41,42 the same could be opted in the studied materials to enhance their applications.…”
Section: Resultsmentioning
confidence: 99%