Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
Hybrid density functional calculations of hyperfine coupling tensor for hole-type defects in MgAl2O4
Introduction
Magnesium aluminate spinel MgAl2O4 exhibits a very high tolerance to irradiation with fast neutrons due to the efficient recombination of primary radiation-induced Frenkel defects - vacancies and interstitials, which makes it a promising material for optical/diagnostics windows in the environment of future fusion reactors. It is generally accepted that the accumulation of radiation-induced structural defects determines the radiation damage and strongly affects the functionality of various optical materials/components. In this connection, the investigation/understanding of the atomic and electronic structure of defects as well as their thermal annealing plays a crucial role.
Recently, it was discussed what happens with the defects formation in neutron-irradiated single crystals of MgAl2O4 [1]. The EPR measurements at room temperature helped to identify the intrinsic structural defects induced by the fast fission neutrons. The obtained values of g-tensor parameters allowed to conclude that the paramagnetic nature of the hole-type centers (called, for simplicity, V-centers in [1]) is supposed to be an O− ion (i.e. a single hole trapped at a regular oxygen ion) located near some negatively charged structural defect. Based on the experimentally measured angular dependencies for different V-centers and their comparison with the calculated ones in the “Easy Spin” program [2], the orientation of paramagnetic centers was determined and the following microstructures of hole-containing centers were proposed [1], [3].
This study showed three different hole-type defects labeled as V1, V2, and V22. In the case of V1-centre a negatively charged defect is situated at the Al3+-site which is the Al vacancy in the formal charge state −2, i.e. V1-centre is a complex + O−. Similarly, the Mg vacancy in the formal charge state −1 is associated with the V2-centre = + O−. Also, the anti-site defect, when Mg2+ occupies the Al3+ position, showed up in the EPR spectra leading to a complex V22 = + O−. It can easily be understood that all the three V-centres are compensated by the formation of holes on oxygen atoms to maintain the electroneutrality condition. The charge state coincides with the supercell charge and should not be confused with the oxidation state like Al3+ and Mg2+ at regular sites.
The DFT calculations of EPR parameters for crystals is still rare in the literature [4], [5]. Previous calculations concerned mainly complex molecules in the cluster model, see, for example, [6], [7]. In the present study we rely on the implementation as suggested in the CRYSTAL17 computer code [8]. Notice that the calculation of g-tensor is not possible in CRYSTAL at the present stage but the HCCs can be calculated as demonstrated in careful study of defects in diamond [5]. Moreover, the DFT calculations could be used to deeper analyze the properties of such defects at atomistic level that is an important complement to experimental data. In previous study of Paudel et al. [9] the anti-site defects and of Jiang et al. [10] the oxygen vacancies in MgAl2O4 were calculated within the so-called DFT + U and G0W0 approach, respectively. Borges et al. [11] studied combinations of oxygen vacancy and anti-sites in different charge states by means of DFT and meta-GGA Becke-Johnson exchange potential. So, all these advanced DFT studies were focused on optical properties of defective MgAl2O4. Recently, the atomic and electronic structure of oxygen interstitial defects in MgAl2O4 was calculated by us using the hybrid DFT calculations [12], [13]. In the present study we decided to extend our hybrid DFT calculations to the V-centres and calculate, for the first time, the HCCs for a comparison with those obtained from the measured EPR spectra.
Section snippets
Computational details
The formalism of linear combination of atomic orbitals (LCAO) combined with the hybrid B3LYP exchange–correlation functional was used in the present study of defects in MgAl2O4. The all-electron basis set of atomic Gaussian type functions in the form 8s-411sp, 8s-511sp and 8s-511sp-1d for O, Mg and Al, respectively, were taken from the CRYSTAL web site (please, see [14] and references therein). The primitive unit cell of MgAl2O4 consists of 14 atoms whereas its conventional unit cell consists
Basic bulk properties of MgAl2O4
Magnesium aluminate MgAl2O4 crystallizes in the spinel structure (space group 227,) which is a face-centred cubic lattice. Its primitive unit cell contains the Mg atoms occupying Wyckoff position 2a (1/8, 1/8, 1/8), Al atoms occupying Wyckoff position 4d (1/2, 1/2, 1/2), and O atoms occupying Wyckoff position 8e (x, x, x) with one free parameter. The calculated lattice constant a of 8.15 Å using the B3LYP functional for the primitive unit cell is little larger than the experimental value
Conclusions
The hybrid B3LYP calculations were performed in order to calculate and analyze properties of hole-type defects in MgAl2O4. The hybrid B3LYP functional reproduced not only the lattice parameters but also the bandgap of MgAl2O4. The main focus was placed on the calculation of V-centres with the single hole trapped on a regular oxygen ion (O−) in accordance with the previous experimental observations. We confirmed that such defects could be present in MgAl2O4. Moreover, the calculated hyperfine
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.
Acknowledgements
This work has been performed within the framework of the EUROfusion Enabling Research project: ENR-MFE19.ISSP-UL-02 “Advanced experimental and theoretical analysis of defect evolution and structural disordering in optical and dielectric materials for fusion application”. The views and opinions expressed herein do not necessarily reflect those of the European Commission. A.L. and V.S. appreciate the support from the Estonian Research Council grant PUT PRG 619.
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