Abstract

$N$-type CdO is a transparent conducting oxide (TCO) which has promise in a number of areas including solar cell applications. In order to realize this potential a detailed knowledge of the electronic structure of the material is essential. In particular, standard density functional theory (DFT) methods struggle to accurately predict fundamental material properties such as the band gap. This is largely due to the underestimation of the Cd 4$d$ binding energy, which results in a strong hybridization with the valence-band (VB) states. In order to test theoretical approaches, comparisons to experiment need to be made. Here, synchrotron-radiation photoelectron spectroscopy (SR-PES) measurements are presented, and comparison with three theoretical approaches are made. In particular the position of the Cd 4$d$ state is measured with hard x-ray PES, and the orbital character of the VB is probed by photon energy dependent measurements. It is found that LDA + U using a theoretical U value of 2.34 eV is very successful in predicting the position of the Cd 4$d$ state. The VB photon energy dependence reveals the O 2$p$ photoionization cross section is underestimated at higher photon energies, and that an orbital contribution from Cd 5$p$ is underestimated by all the DFT approaches.

Highlights

  • CdO is a rocksalt metal oxide which is amenable to n-type doping resulting in high conductivity and optical transparency

  • The VB region shown in panels (g)–(i) of Fig. 3 exhibits a two peak structure which is correctly reproduced by all the density functional theory (DFT) functionals

  • The VB electronic structure of CdO has been investigated with synchrotron-radiation photoelectron spectroscopy (SR-PES), and comparisons to three DFT functionals have been made

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Summary

INTRODUCTION

CdO is a rocksalt metal oxide which is amenable to n-type doping resulting in high conductivity and optical transparency. There have been several theoretical attempts to correct this problem including the use of hybrid functionals [9,10] and GW quasiparticle calculations [11,12] These approaches have had some success in predicting the location of the shallow Cd 4d states and the band gap; they are computationally more complex and less widely applied. An alternative approach is LDA + U [13,14,15], where an on-site, orbital dependent Coulomb term is added to the local density approximation (LDA) potential This allows the position of the Cd 4d states to be corrected and should improve the associated theoretical predictions. Three DFT functionals were chosen (LDA, PBE-GGA, and LDA + U), due to their widespread availability and relative computational simplicity

EXPERIMENTAL DETAILS
Density functional theory
Experimental comparison
Computational results
CONCLUSIONS
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