Abstract

We investigate the stability of self-trapped holes (STHs) and the acceptor levels of substitutional Mg and N impurities in $\ensuremath{\alpha}$-, $\ensuremath{\beta}$-, $\ensuremath{\delta}$-, and $\ensuremath{\varepsilon}\text{\ensuremath{-}}{\mathrm{Ga}}_{2}{\mathrm{O}}_{3}$ using first-principles calculations based on the hybrid functional approach to assess their $p$-type dopability. When Fock-exchange and screening parameter values in the Heyd-Scuseria-Ernzerhof (HSE) hybrid functional are optimized to satisfy the generalized Koopmans' theorem for a STH level in $\ensuremath{\beta}\text{\ensuremath{-}}{\mathrm{Ga}}_{2}{\mathrm{O}}_{3}$, the band gap is slightly overestimated, while functionals that well reproduce the band gap show slight convex behavior against the fractional electron number. However, the absolute position of the STH level at a fixed geometry is nearly independent of the parameter value, showing that the results are robust as long as the STH geometry and localized electronic nature are appropriately described and the band edges are well reproduced. In all of the polymorphs, holes localize with high self-trapping energies rather than being delocalized. Furthermore, both Mg and N impurities introduce polaronic acceptor states, and their acceptor levels lie far above the valence band maximum in all the polymorphs. Thus, the $p$-type doping of the four ${\mathrm{Ga}}_{2}{\mathrm{O}}_{3}$ polymorphs seems unfeasible in terms of the STH formation and the related deep, polaronic acceptor nature of the Mg and N impurities.

Highlights

  • With a wide band gap of 4.9 eV and n-type dopability [1,2], β-Ga2O3 is a promising deep ultraviolet (UV) transparent conductor for applications such as power electronic devices and solar blind UV photodetectors [3,4,5,6,7,8]

  • We have investigated the stability of self-trapped holes (STHs) and the acceptor levels of Mg and N impurities using the HSE hybrid functional to assess the p-type dopability of α, β, δ, and ε-Ga2O3

  • We found that the parameter values that well meet the generalized Koopmans’ theorem (gKT) condition slightly overestimate the band gap, whlie HSE(0.35, 0.21) shows slightly convex behavior

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Summary

Introduction

With a wide band gap of 4.9 eV and n-type dopability [1,2], β-Ga2O3 is a promising deep ultraviolet (UV) transparent conductor for applications such as power electronic devices and solar blind UV photodetectors [3,4,5,6,7,8]. Previous first-principles studies on the p-type dopability of β-Ga2O3 have revealed a lack of shallow acceptors [15,16] and formation of self-trapped holes (STHs) [17,18,19], both of which hinder efficient p-type doping. The relatively localized valence states could lead to STH formation and, low-hole mobility [17]. This is one reason p-type doping is challenging for many oxides. Formation of deep acceptor states is closely related to STH stability, as such deep states typically result from polaronic hole trapping [16,27,28,29,30].

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