Piezoelectric properties of [Ga.sub.2][O.sub.3]: a first-principle study

The compounds exhibit piezoelectricity, which demands to break inversion symmetry, and then to be a semiconductor. For [Ga.sub.2][O.sub.3], the orthorhombic case ([epsilon]-[Ga.sub.2][O.sub.3]) of common five phases breaks inversion symmetry. Here, the piezoelectric tensor of [epsilon]-[Ga.sub.2][O....

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Bibliographic Details
Published inThe European physical journal. B, Condensed matter physics Vol. 93; no. 1
Main Authors Guo, San-Dong, Du, Hui-Min
Format Journal Article
LanguageEnglish
Published Springer 15.04.2020
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Summary:The compounds exhibit piezoelectricity, which demands to break inversion symmetry, and then to be a semiconductor. For [Ga.sub.2][O.sub.3], the orthorhombic case ([epsilon]-[Ga.sub.2][O.sub.3]) of common five phases breaks inversion symmetry. Here, the piezoelectric tensor of [epsilon]-[Ga.sub.2][O.sub.3] is reported by using density functional perturbation theory (DFPT). To confirm semiconducting property of [epsilon]-[Ga.sub.2][O.sub.3], its electronic structures are studied by using generalized gradient approximation (GGA) and Tran and Blaha's modified Becke and Johnson (mBJ) exchange potential. The gap value of 4.66 eV is predicted with mBJ method, along with the effective mass tensor for electron at the conduction band minimum (CBM) [about 0.24 [m.sub.0]]. The mBJ gap is very close to the available experimental value. The elastic tensor [C.sub.ij] are calculated by using the finite difference method (FDM), and piezoelectric stress tensor [e.sub.ij] are attained by DFPT, and then piezoelectric strain tensor [d.sub.ij] are calculated from [C.sub.ij] and [e.sub.ij]. In this process, average mechanical properties of [epsilon]-[Ga.sub.2][O.sub.3] are estimated, such as bulk modulus, Shear modulus, Young's modulus and so on. The calculated [d.sub.ij] are comparable and even higher than commonly used piezoelectric materials such as a-quartz, ZnO, AlN and GaN.
ISSN:1434-6028
1434-6036
DOI:10.1140/epjb/e2019-100516-6