2023
DOI: 10.12693/aphyspola.143.36
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Structural, Thermodynamic and Magneto-Electronic Properties of Cd0.75Cr0.25Se and Zn0.75Cr0.25S: An <i>Ab-Initio</i> Study

Abstract: Using the full-potential linearized augmented plane wave plus local orbital method based on spinpolarized density functional theory, we investigate the parameters of the structure, the electronic, magnetic, and thermodynamic properties of cubic zinc-blende Cd0.75Cr0.25Se and Zn0.75Cr0.25S ordered ferromagnetic materials. We adopt the Perdew-Burke-Ernzerhof generalized gradient approximation and the modified Becke-Johnson exchange potential for the exchange-correlation energy and potential. Furthermore, the eff… Show more

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Cited by 3 publications
(2 citation statements)
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“…We observe that the bulk modulus B of CaO compound increases with increasing pressure up to 65.2 GPa. The results are consistent with the values reported for CdSe, Cd0.75Cr0.25Se, ZnS, and Zn0.75Cr0.25S materials [29]. Compared with the bulk modulus B at equilibrium, our obtained data of B using the experimental elastic constants measured by Speziale et al [6] are somewhat larger than both the ab initio plane-wave pseudopotential DFT method [2] and semi-empirical approach [5] at high pressure.…”
Section: Theory Results and Discussionsupporting
confidence: 91%
“…We observe that the bulk modulus B of CaO compound increases with increasing pressure up to 65.2 GPa. The results are consistent with the values reported for CdSe, Cd0.75Cr0.25Se, ZnS, and Zn0.75Cr0.25S materials [29]. Compared with the bulk modulus B at equilibrium, our obtained data of B using the experimental elastic constants measured by Speziale et al [6] are somewhat larger than both the ab initio plane-wave pseudopotential DFT method [2] and semi-empirical approach [5] at high pressure.…”
Section: Theory Results and Discussionsupporting
confidence: 91%
“…8 that the CV of Cu2ZnSnS4 material increases exponentially with the temperature for T < 400 K, while for high temperature, it approaches the DuLong-Petit limit, indicating that at high temperature, all phonon modes are sufficiently excited by the thermal energy [34]. Due to general laws of thermodynamics and the same nature of materials as semiconductors, it can be observed that similar qualitative behaviors from the quantitative point of view have been reported for CV versus temperature for ScP material [32], copper chloride (CuCl) and copper bromide (CuBr) compounds [34], group Ⅲ-phosphide semiconducting materials [35], for boron antimonide (BSb) compound in cubic zinc-blende structure [36], and for both Cd0.75Cr0.25Se and Zn0.75Cr0.25S ternary materials [37]. At 298 K, the constant volume heat capacity CV was found to be at around 376.44 Jmol -1 K -1 .…”
Section: Constant Volume Heat Capacitysupporting
confidence: 64%