4.6 Article

A computational study of the thortveitite structure of zinc pyrovanadate, Zn2V2O7, under pressure

Journal

RSC ADVANCES
Volume 13, Issue 25, Pages 17212-17221

Publisher

ROYAL SOC CHEMISTRY
DOI: 10.1039/d3ra02426a

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We conducted a pressure-driven study on zinc pyrovanadate (Zn2V2O7) using the density functional theory (DFT). Zn2V2O7 exists in a monoclinic structure (alpha-phase) under normal pressure. Four high-pressure phases (beta, gamma, kappa, and delta) were observed at 0.7, 3.8, 4.8, and 5.3 GPa, respectively. These phases exhibit mechanical stability, elastic anisotropy, and malleability. The compressibility of Zn2V2O7 is higher compared to other meta- and pyrovanadates. The energy dispersion analysis suggests that these phases are indirect band gap semiconductors with wide band gap energies. The band gap energies generally decrease with increasing pressure, except for the kappa-phase. The effective masses and band gap values obtained from the band structures are consistent with the optical absorption spectra.
We performed a pressure-driven study of zinc pyrovanadate, Zn2V2O7, using the first-principles approach under the framework of density functional theory (DFT). Zn2V2O7 crystalizes in a monoclinic (alpha-phase) structure with the space group C2/c at ambient pressure. In comparison with the ambient phase, there are four different high-pressure phases, namely beta, gamma, kappa and delta, found at 0.7, 3.8, 4.8 and 5.3 GPa, respectively. The detailed crystallographic analysis as well as their structures is consistent with the theory and experiment reported in the literature. All phases including the ambient phase are mechanically stable, elastically anisotropic and malleable. The compressibility of the studied pyrovanadate is higher than that of the other meta- and pyrovanadates. The energy dispersion of these studied phases reveals that they are indirect band gap semiconductors with wide band gap energies. The band gap energies follow a reduced trend with pressure except the kappa-phase. The effective masses for all of these studied phases were computed from their corresponding band structures. The values of energy gaps obtained from the band structures are almost similar to the optical band gap obtained from the optical absorption spectra, as estimated by the Wood-Tauc theory.

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