Malays. J. Anal. Sci. Volume 30 Number 1 (2026): 1602
Research Article
Structural,
electronic, and optical properties of N/Y-codoped anatase TiO2: A first-principles
investigation
Noor ‘Aisyah Johari1,*,
Norjuliyati Hamzah1, Ahmad Fuzairi Ahmad Faizal1, Nur Hamizah
Mohd Zaki2,3, Ab Malik Marwan Ali2,3, Oskar Hasdinor Hassan3,4,
Muhd Zu Azhan Yahya5, and Mohamad Fariz Mohamad Taib2,3
1Centre of Foundation Studies,
Universiti Teknologi MARA (UiTM), 43800 Dengkil, Selangor, Malaysia
2Faculty of Applied Sciences, Universiti Teknologi MARA
(UiTM), 40450 Shah Alam, Selangor, Malaysia
3Institute of Sciences, Universiti Teknologi MARA (UiTM),
40450 Shah Alam, Selangor, Malaysia
4Department of Industrial Ceramic, Faculty of Art and Design,
Universiti Teknologi MARA (UiTM), 40450 Shah Alam, Selangor, Malaysia
5Faculty of Defence Science and Technology, Universiti
Pertahanan Nasional Malaysia (UPNM), 57000 Kuala Lumpur, Malaysia
*Corresponding author: noorai2902@uitm.edu.my
Received: 10 June 2025; Revised: 1
December 2025; Accepted: 1 December 2025; Published: 28 February 2026
Abstract
The influence of N/Y codoping on the structural, electronic,
and optical characteristics of anatase TiO2 is investigated using
density function theory. The calculated band gaps are 2.149 eV for pure TiO2,
1.534 eV for N-doped TiO2, 2.142 eV for Y-doped TiO2, and
1.880 eV for N/Y-codoped TiO2. The slightly lower value of pure TiO2
compared to the experimental band gap (~3.2 eV) is attributed to the well-known
underestimation effect of the GGA-PBEsol functional in DFT calculations. The
valence band of pure TiO2 is mainly composed of O 2p states,
and the conduction band is mainly composed of Ti 3d states. For N-doped
TiO2, the valence band is mainly occupied by N 2p states,
which are higher than that of the O 2p states, which can narrow the band
gap. Y doping will introduce 4d states, which are involved in the
conduction band. As for N/Y codoped, the valence band is mainly occupied by N 2p
and O 2p states, while the conduction band is predominantly occupied by
Y 4d and Ti 3d states. Furthermore, N-doped TiO2, Y-doped TiO2,
and N/Y-codoped TiO2 will result in a red-shift of the absorption
edge compared with the pure TiO2 and significantly enhanced in the
visible light region.
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