Quasiparticle self-consistent GW band structures and high-pressure phase transitions of LiGaO2 and NaGaO2

Santosh Kumar Radha, Amol Ratnaparkhe, and Walter R. L. Lambrecht
Phys. Rev. B 103, 045201 – Published 6 January 2021

Abstract

Quasiparticle self-consistent GW calculations are presented for the band structures of LiGaO2 and NaGaO2 in the orthorhombic Pna21 tetrahedrally coordinated crystal structures, which are closely related to the wurtzite structure of ZnO. Symmetry labeling of the bands near the gap is carried out, and effective-mass tensors are extracted for the conduction-band minimum and crystal-field split valence-band maxima (VBM) at Γ. The gap is found to be direct at Γ and is 5.81 eV in LiGaO2 and 5.46 eV in NaGaO2. Electron-phonon coupling zero-point normalization is estimated to lower these gaps by about 0.2±0.1 eV. Optical response functions are calculated within the independent-particle long-wavelength limit, and they show the expected anisotropy of the absorption onsets due to the crystal-field splitting of the VBM. The results show that both materials are promising candidates as ultrawide-gap semiconductors with wurtzite-based tetrahedrally bonded crystal structures. Direct transitions from the lowest conduction band to higher bands, relevant to n-type doped material and transparent conduction applications, are found to start only above 3.9 eV and are allowed for only one polarization, and several higher band transitions are forbidden by symmetry. Alternative crystal structures, such as R3¯m and a rocksalt-type phase with a tetragonally distorted P4/mmm spacegroup, both with octahedral coordination of the cations, are also investigated. They are found to have higher energy but about 20% smaller volume per formula unit. The transition pressures to these phases are determined, and for LiGaO2 they are found to be in good agreement with experimental studies. The R3¯m phase also has a comparably high but slightly indirect band gap, while the rocksalt-type phase is found to have a considerably smaller gap of about 3.1 eV in LiGaO2 and 1.0 eV in NaGaO2.

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  • Received 28 October 2020
  • Accepted 18 December 2020

DOI:https://doi.org/10.1103/PhysRevB.103.045201

©2021 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Santosh Kumar Radha, Amol Ratnaparkhe, and Walter R. L. Lambrecht

  • Department of Physics, Case Western Reserve University, 10900 Euclid Avenue, Cleveland, Ohio 44106-7079, USA

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Issue

Vol. 103, Iss. 4 — 15 January 2021

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