Influence of Hubbard U on the Structural and Electronic Properties of Pure and La-Doped ZnO

Authors

  • Muhd Aman Haikal Razali Faculty of Applied Sciences, Universiti Teknologi MARA (UiTM), 40450 Shah Alam, Selangor, Malaysia Author
  • Nur Ain Nabilah Mohamad Nor Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia Author
  • Wan Hazeeq Azizi Wan Khairul Annuar Faculty of Applied Sciences, Universiti Teknologi MARA (UiTM), 40450 Shah Alam, Selangor, Malaysia Author
  • Mohd Hazrie Samat Ionic Materials and Devices (iMADE), Institute of Science, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia Author
  • Nur Hamizah Mohd Zaki Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia Author
  • Ahmad Firdaus Che Omar Ionic Materials and Devices (iMADE), Institute of Science, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia Author
  • Mohd Fariz Mohamad Taib Faculty of Applied Sciences, Universiti Teknologi MARA (UiTM), 40450 Shah Alam, Selangor, Malaysia Author
  • Ferry Iskandar Department of Physics, Faculty of Mathematics and Natural Sciences, Institut Teknologi Bandung, Jl. Ganesha 10, 40132 Bandung, Indonesia Author
  • Oskar Hasdinor Hassan Ionic Materials & Devices (iMADE) Research Laboratory, Institute of Science, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia Author

DOI:

https://doi.org/10.66514//ssst32-2-121-134

Keywords:

Density functional theory, electronic properties, La-doped ZnO, Hubbard U, structural properties, ZnO

Abstract

The lattice parameters, average bond length, band structure and density of states (DOS) of pure ZnO and La-doped ZnO were calculated using the density functional theory (DFT) with the addition of Hubbard U (DFT+U) correction method. Lanthanum, La is a p-type dopant that might be viewed as a practical method for improving a piezoelectric nanogenerator's performance. The calculated lattice parameters and volume of pure ZnO expanded after La doping which are a=b=3.251 Å, c=5.208 Å and V= 48.346 Å3. The Zn-O bond length of La-doped ZnO is higher than that of pure ZnO which makes the La-doped ZnO having stronger bonding than pure ZnO. The calculated band gap of pure ZnO was 3.415 eV and for La-doped ZnO, the band gap shows an increases to 3.457 eV. The calculated band gap approaches the experimental band gap with the implementation of Hubbard U at Ud at Zn and La sites and Up at O sites. The density of states (DOS) of both pure ZnO and La-doped ZnO were conducted to determine the contribution of s, p and d orbitals that appear in the minimum conduction band and maximum valence band. As a result, we believe that our findings will be useful in understanding the doping impact in ZnO and will motivate further theoretical research.

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Published

30-09-2024