2019
DOI: 10.1016/j.jallcom.2018.08.314
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Ab-initio studies of electronic, structural and thermophysical properties of the Sr2TiMoO6 double perovskite

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Cited by 18 publications
(7 citation statements)
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“…For this purpose, these properties were calculated as a function of temperature, under the application of several pressure values up to 35 GPa, using as a starting point the state equation, and following the quasi-harmonic approximation of the Debye model. [29]. In figure 7, the results of the specific heat at constant volume (figure 7(a)) and at constant pressure (figure 7(b)) as a function of the temperature up to T=1500 K and under the application of pressures up to 35 GPa are exemplified.…”
Section: Resultsmentioning
confidence: 99%
“…For this purpose, these properties were calculated as a function of temperature, under the application of several pressure values up to 35 GPa, using as a starting point the state equation, and following the quasi-harmonic approximation of the Debye model. [29]. In figure 7, the results of the specific heat at constant volume (figure 7(a)) and at constant pressure (figure 7(b)) as a function of the temperature up to T=1500 K and under the application of pressures up to 35 GPa are exemplified.…”
Section: Resultsmentioning
confidence: 99%
“…The variation of thermodynamic properties as a function of temperature and pressure can give relevant information for the understanding of the macroscopic behaviours exhibited by the material. Although this dependence of thermophysical properties has been carried out for perovskites of various structures [14,64], there are no references in the literature for the Dy 2 Bi 2 Fe 4 O 12 material. The Debye quasi-harmonic approximation was applied from the equation of state to obtain the specific heat at both constant volume and constant pressure in the temperature regime between 0 K and 1200 K, as exemplified in figure 4.…”
Section: Thermophysical Propertiesmentioning
confidence: 99%
“…Figures 4(a) and (b) show an identical behaviour of C V (T) and C P (T) up to a temperature value close to 600 K for all applied pressure values. Above this temperature value, while C V reaches the Dulong-Petit limit (L DP = 492 J mol −1 K), above which there is no temperature dependence, C P (T) still continues to increase with augmenting temperature values until it reaches 525 J mol −1 K at T = 1200 K. Interestingly, the L DP seems to be dependent on crystal symmetries, since this value does not exceed 240 J mol −1 K in cubic double perovskites [15,51] but reaches values higher than 475 J mol −1 K in less symmetric crystals [6,14]. This can take place because crystalline asymmetry introduces anharmonicity effects which end up producing anharmonic contributions on the thermodynamical functions that are increased the more complex the structures of the materials studied [65,66].…”
Section: Thermophysical Propertiesmentioning
confidence: 99%
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“…Additionally, considering that in materials science one of the sure ways to classify materials is the electronic structure, which can be theoretically determined from ab initio methods, in this work the density functional theory (DFT) is applied to determine the band structure and the density of electronic states of the material, since this method allows us to identify the eventual occurrence of bandgaps, as well as the types of hybridization between orbitals and electronic bands that give rise to the macroscopic measurable behaviors. 25,26…”
Section: Introductionmentioning
confidence: 99%