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Structural stability, band structure and magnetic properties of ZnS and Zn0.75Cr0.25S under pressure

[Display omitted] ► Zn0.75Cr0.25S is more anisotropic and is easier to deform than ZnS. ► ZnS can exist stably under pressure up to 10GPa with increasing direct band gap. ► The structural stability can be kept up to 5GPa for the case of Zn.075Cr0.25S. ► Zn.075Cr0.25S is half metallic with Eg and Eg-...

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Bibliographic Details
Published in:Journal of alloys and compounds 2013-02, Vol.549, p.184-189
Main Authors: Huang, Yu-hong, Jie, Wan-qi, Zhou, Yan, Zha, Gang-qiang
Format: Article
Language:English
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Summary:[Display omitted] ► Zn0.75Cr0.25S is more anisotropic and is easier to deform than ZnS. ► ZnS can exist stably under pressure up to 10GPa with increasing direct band gap. ► The structural stability can be kept up to 5GPa for the case of Zn.075Cr0.25S. ► Zn.075Cr0.25S is half metallic with Eg and Eg-HM increasing with P below 6GPa. ► Δx(d) and Δx(pd) decrease as pressure increases. Due to the significant luminescent properties of ZnS and the half metallic features of Cr doped ZnS (Zn0.75Cr0.25S), many researches have been done to make possible the use of these materials in optical and spintronic devices. The environmental conditions, such as, high pressure and high temperature, are crucial for the device service, however, it is difficult to exploit this issue from the experimental aspect. Therefore, spin-polarized first-principle calculations were performed to study the structural stability, band structure and magnetic properties of zincblende ZnS and Zn0.75Cr0.25S under pressure. It is shown that ZnS can exist stably under pressure up to 10GPa, while Zn0.75Cr0.25S becomes unstable under a pressure of 5GPa or so. The bulk modulus (BH), Poisson ratio (v) and anisotropic parameter (A) of ZnS and Zn0.75Cr0.25S increase with pressure, but the shear modulus (GH) decreases. BH and GH of Zn0.75Cr0.25S are smaller than those of ZnS, while v and A of Zn0.75Cr0.25S are larger than those of ZnS. Both ZnS and Zn0.75Cr0.25S behave in a ductile manner, while Zn0.75Cr0.25S is more anisotropic and is easier to induce deformation than ZnS. As for ZnS, the direct band structure is kept but the band gap increases gradually with the pressure. As for Zn0.75Cr0.25S, the half metallic features are maintained up to a pressure of 10GPa, but both the band gap for minority spin and the half metallic band gap have the largest values under 6Pa. The spin exchange splitting energy Δx(d) and Δx(pd) decrease with the increase of pressure. The negative values of Δx(pd) under pressure imply that the effective potential (Eep) of the minority spin is more attractive than that of majority spin.
ISSN:0925-8388
1873-4669
DOI:10.1016/j.jallcom.2012.09.031