Piezoelectric properties of $\mathrm{G}{\mathrm{a}}_2{\mathrm{O}}_3$: a first-principle study

Abstract

The compounds exhibit piezoelectricity, which demands to break inversion symmetry, and then to be a semiconductor. For $\mathrm{G}{\mathrm{a}}_2{\mathrm{O}}_3$, the orthorhombic case ($\epsilon$-$\mathrm{G}{\mathrm{a}}_2{\mathrm{O}}_3$) of common five phases breaks inversion symmetry. Here, the piezoelectric tensor of $\epsilon$-$\mathrm{G}{\mathrm{a}}_2{\mathrm{O}}_3$ is reported by using density functional perturbation theory (DFPT). To confirm semiconducting properties of $\epsilon$-$\mathrm{G}{\mathrm{a}}_2{\mathrm{O}}_3$, 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 the effective mass tensor for electrons at the conduction band minimum (CBM) [about 0.24 $m_0$]. The mBJ gap is very close to the available experimental value. The elastic tensor $C_{ij}$ and piezoelectric stress tensor $e_{ij}$ are attained by DFPT, and then piezoelectric strain tensor $d_{ij}$ are calculated from $C_{ij}$ and $e_{ij}$. In this process, average mechanical properties of $\epsilon$-$\mathrm{G}{\mathrm{a}}_2{\mathrm{O}}_3$ are estimated, such as bulk modulus, Shear modulus, Young's modulus and so on. The calculated $d_{ij}$ are comparable and even higher than commonly used piezoelectric materials such as $\alpha$-quartz, ZnO, AlN and GaN.

arXiv comment5pages, 2 figures

References in corpus (5)

• Necessary and Sufficient Elastic Stability Conditions in Various Crystal Systems
• Systematic treatment of displacements, strains and electric fields in density-functional perturbation theory
• Polarization-based calculation of the dielectric tensor of polar crystals
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• First-principles calculation of the piezoelectric tensor d of III-V nitrides

Cited by in corpus (1)

• Piezoelectric properties of substitutionally doped $\beta$-Ga${}_2$O${}_3$