Abstract

The p-type semiconductors Cu2O and ZnRh2O4 have been under investigation for potential applications as transparent conducting oxides. Here, we re-evaluate their structural, electronic, and optical properties by means of first-principles calculations employing density functional theory and a recently introduced self-consistent hybrid functional approach. Therein, the predefined fraction α of Hartree–Fock exact exchange is determined self-consistently via the inverse of the dielectric constant ε∞. The structural, electronic, and optical properties will be discussed alongside experimental results, with a focus on possible technological applications.

Highlights

  • Transparent conducting oxides (TCOs) are one important building block of current technological devices, ranging from various display applications to solar cells

  • The present work focuses on two identified examples for p-type TCOs, namely cuprous oxide (Cu2 O) and ZnRh2 O4

  • Cu2 O crystallises in the cubic crystal structure, whereas ZnRh2 O4 crystallises in the so-called normal spinel crystal structure, respectively, similar to ZnFe2 O4 [2], but at variance to NiFe2 O4 and CoFe2 O4 which crystallise in the inverse spinel structure [3]

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Summary

Introduction

Transparent conducting oxides (TCOs) are one important building block of current technological devices, ranging from various display applications to solar cells. Subsequent first-principles calculations of the whole spinel series ZnM2 O4 (M = Co, Rh, and Ir) tried to identify their conduction mechanism, i.e., hole or polaron conduction [8,9,10] These first-principles calculations employed a range of (semi)local and hybrid exchange and correlation functionals to investigate the structural, electronic, and optical properties of ZnRh2 O4 , respectively. The recent development of a self-consistent hybrid functional [12] provided the motivation for the current work, namely to re-evaluate the structural, electronic, and optical properties of Cu2 O and ZnRh2 O4 , similar to other crystalline [13,14] and amorphous [15,16].

Theoretical Background
Structural Properties
Electronic and Optical Properties
Summary and Outlook
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