Research paperEffects of oxygen vacancy on the magnetic properties of Mn(II)-doped anatase TiO2
Graphical abstract
Introduction
As a promising wide-band gap semiconductor, titanium dioxide (TiO2) has received much attention due to its outstanding performance in the photonic, electronic, and magnetic applications [1], [2], [3], [4]. Many investigations found that doping with 3d transition metal (TM) induce the magnetic moment in TiO2 [5], [6], [7], [8], [9], [10], [11], even if the origin of the magnetism in 3d TM-doped TiO2 remains confusing. For instance, some different results were observed in Mn-doped TiO2. Bhattacharyya et al. [5] reported that the room temperature (RT) ferromagnetism behavior of Ti1-xMnxO2 nanocrystals is dependent on the Mn doping concentration. Hong et al. [6] demonstrated that Mn dopant did not play an important role in Mn-doped TiO2 thin films. When the dopant concentration is below 5%, the Mn atom enhances the magnetic moment, whereas the Mn doping destroys the ferromagnetism of the host if the dopant content increases to larger than 10% [6]. Moreover, some researches showed that the undoped TiO2 thin films can also exhibit RT ferromagnetism. Vacuum annealing enhances the RT ferromagnetic signal, and the subsequent annealing in air can reduce it, which illustrates that the observed RT ferromagnetism in undoped TiO2 thin films is connected with oxygen vacancies [7].
On the other hand, several different results [8], [9] have been reported by someone who use the First-principles to investigate the magnetism of TiO2. Errico et al. [8] investigated the ferromagnetism of Mn-, Fe-, Co–, and Ni-doped TiO2 by first-principles calculations, and found that the spin-polarization mainly occurs at the impurity sites, and the magnetic moments of the impurities are independent of the impurity concentration. Li et al. [9] proposed that O divacancy, Ti single vacancy and divacancy could introduce the local magnetic moments in undoped TiO2.
The recent research by Ahmed confirmed that the interactions between manganese ions and oxygen vacancies could cause the RT ferromagnetism in Mn-doped TiO2 [10]. However, Duhalde et al. [11] prepared Ti0.9TM0.1O2-δ (TM = Mn, Fe, Co, Ni, Cu) thin films by pulsed laser deposition, and found that Ti0.9Mn0.1O2-δ film has no ferromagnetism signal. Up to now, no rigorous theoretical model can determine the roles of Mn(II) ions in Ti1-xMn(II)xO2 system, and the correlation between magnetism and oxygen vacancies remains controversial. Therefore, it is necessary to give a detailed description of the magnetic properties of Mn(II)-doped TnO2 and understand reasonably the effects of VO on the magnetism of this doping system. In addition, compared with the traditional DFT calculation, the hybrid function could get more accurate results [12]. The calculated parameter testing is also one of the work in this paper.
Section snippets
Computational methods
The Vienna ab initio simulation package (VASP) was performed to calculate with the Heyd-Scuseria-Ernzerhof (HSE) function. An energy cutoff of 400 eV was set to describe the electronic wave function. For the k-point integration, the 3 × 3 × 3 mesh was enough to get an accurate result. The calculation would stop when the force was reduced to within 0.01 eV/Å. The good convergence results can get with these parameters. The 2 × 2 × 1 anatase TiO2 (a-TiO2) supercell was established to carry on
Results and discussion
The stoichiometric a-TiO2 supercell is calculated as a reference, and the optimized model has little change, as shown in Fig. 1(a). It should be noted that the HSE function can improve the calculation accuracy by the fraction of exact exchange (AEXX) which directly affects the band gap and the energy of a-TiO2. In order to get a more accurate band gap, we set different AEXX values, and the results are shown in Fig. 1(b). With the increase of the AEXX value, the band gap increases linearly and
Conclusion
We studied the magnetism of Mn(II)-doped a-TiO2 with and without VO by HSE hybrid functional method. The undoped a-TiO2 is nonmagnetic, the introduction of Mn(II) dopants can cause a-TiO2 to have a local magnetic moment, which is in direct proportion to the doped concentrations. The type of preferential magnetic coupling in Mn(II)-doped a-TiO2 depends upon the distance between two Mn(II), and AFM coupling is more favorable in most cases. The introduction of increases the local magnetic
CRediT authorship contribution statement
Min Zhou: Formal analysis, Investigation, Data curation, Writing - original draft. Yatong Wang: Formal analysis, Writing - original draft. Yongjia Zhang: Conceptualization, Methodology, Validation, Resources, Writing - original draft, Writing - review & editing, Project administration. Li Sun: Formal analysis, Resources, Project administration. Wentao Hao: Formal analysis, Resources, Project administration. Ensi Cao: Formal analysis, Resources, Project administration. Zhi Yang: Software,
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgments
This work was supported by National Natural Science Foundation of China (Grant no. 11604234, 11404236, and 51602214).
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