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Stability, electronic quantum states, and magnetic interactions of Er 3+ ions in Ga 2 ⁢O 3

Here, we report an ab initio study of phase stability, defect formation, electronic structure, and multiple magnetic, Dzyaloshinskii-Moriya, optical, hyperfine, and crystal field interactions in erbium (Er)-doped wide band gap 𝛼- and 𝛽-gallium oxides (Ga 2 ⁢O 3 ), critically important to make a foundation for both optoelectronic and quantum information applications. The chemical, structural, mechanical, and dynamical stabilities of the pristine phases are confirmed from respective negative formation energies, negative cohesive energies, favorable elastic constants, and positive phonon frequencies. The phonon dispersions indicate that the Ga-O bonds are uniform in the 𝛼-phase, while they vary in the 𝛽-phase due to the anisotropic polyhedral movement. The defect formation energy analysis confirms that both Er-doped 𝛼- and 𝛽−Ga 2 ⁢O 3 prefer Er 3+ (neutral) state. The underestimated band gaps of the pristine phases from standard density functional theory (DFT) calculations as compared to experimental values are corrected by employing the hybrid functional calculations, resulting in the indirect band gaps of 5.21 eV in 𝛼−Ga 2 ⁢O 3 and 4.94 eV in 𝛽−Ga 2 ⁢O 3 . The site preference energy analysis indicates partial occupation of Er in the octahedral site of Ga. The anisotropic nature of hyperfine tensor coefficients of Er is similar in both phases, which may be due to the occupation of Er in the same octahedral Ga site. On the other hand, the calculated magnetic exchange interaction between two Er dopants is negative for 𝛼 and positive for 𝛽, indicating an antiferromagnetic (AFM) ground state in the former and a ferromagnetic (FM) ground state in the latter. Large values of Dzyaloshinskii-Moriya interactions (DMIs) are obtained along the 𝑥 direction in the 𝛼 and along the 𝑦 direction in the 𝛽. The large DMI may support exotic magnetic textures, a promising direction for spintronic applications. The analysis of dielectric constants and refractive indices of both pristine and Er-doped phases shows a good agreement with available experimental values. The calculated optical anisotropy is slightly higher in 𝛽 than those in 𝛼, which is due to the involvement of lower symmetry in 𝛽. The crystal field coefficients (CFCs) calculated from DFT are used to analyze 4⁢𝑓 multiplets and 4⁢𝑓 −4⁢𝑓 transitions. Thus calculated lowest energy level of the first excited state to the lowest energy level of the ground state is about 1.53 µ⁢m, which is in a good agreement with available experiments, and it falls within the quantum telecommunication wavelength range.

3-dimensional systems↗

Materials Data on Ga2O3 by Materials Project

Ga2O3 is Corundum structured and crystallizes in the trigonal R-3c space group. The structure is three-dimensional. Ga3+ is bonded to six equivalent O2- atoms to form a mixture of distorted corner, edge, and face-sharing GaO6 octahedra. The corner-sharing octahedra tilt angles range from 49–61°. There are three shorter (1.95 Å) and three longer (2.11 Å) Ga–O bond lengths. O2- is bonded to four equivalent Ga3+ atoms to form a mixture of distorted corner and edge-sharing OGa4 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Ga2O3 by Materials Project

Ga2O3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. there are two inequivalent Ga3+ sites. In the first Ga3+ site, Ga3+ is bonded in a 6-coordinate geometry to six O2- atoms. There are two shorter (1.96 Å) and four longer (2.17 Å) Ga–O bond lengths. In the second Ga3+ site, Ga3+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing GaO6 octahedra. The corner-sharing octahedral tilt angles are 58°. There are four shorter (1.98 Å) and two longer (2.08 Å) Ga–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to four Ga3+ atoms. In the second O2- site, O2- is bonded to four Ga3+ atoms to form corner-sharing OGa4 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Ga2O3 by Materials Project

Ga2O3 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Ga3+ sites. In the first Ga3+ site, Ga3+ is bonded to six O2- atoms to form GaO6 octahedra that share corners with seven equivalent GaO4 tetrahedra and edges with four equivalent GaO6 octahedra. There are a spread of Ga–O bond distances ranging from 1.97–2.11 Å. In the second Ga3+ site, Ga3+ is bonded to four O2- atoms to form GaO4 tetrahedra that share corners with seven equivalent GaO6 octahedra and corners with two equivalent GaO4 tetrahedra. The corner-sharing octahedra tilt angles range from 56–64°. There is three shorter (1.86 Å) and one longer (1.89 Å) Ga–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three Ga3+ atoms. In the second O2- site, O2- is bonded to four Ga3+ atoms to form a mixture of distorted edge and corner-sharing OGa4 tetrahedra. In the third O2- site, O2- is bonded in a trigonal planar geometry to three Ga3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on GaO by Materials Project

GaO is Wurtzite structured and crystallizes in the hexagonal P6_3mc space group. The structure is three-dimensional. Ga2+ is bonded to four equivalent O2- atoms to form corner-sharing GaO4 tetrahedra. There are three shorter (2.08 Å) and one longer (2.15 Å) Ga–O bond lengths. O2- is bonded to four equivalent Ga2+ atoms to form corner-sharing OGa4 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Ga3O5 by Materials Project

Ga3O5 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are three inequivalent Ga sites. In the first Ga site, Ga is bonded to four O atoms to form GaO4 tetrahedra that share corners with four equivalent GaO6 octahedra and corners with three equivalent GaO4 tetrahedra. The corner-sharing octahedra tilt angles range from 51–62°. There is one shorter (1.83 Å) and three longer (1.87 Å) Ga–O bond length. In the second Ga site, Ga is bonded to six O atoms to form GaO6 octahedra that share corners with eight GaO4 tetrahedra and edges with two equivalent GaO6 octahedra. There are four shorter (1.98 Å) and two longer (2.03 Å) Ga–O bond lengths. In the third Ga site, Ga is bonded to four O atoms to form GaO4 tetrahedra that share corners with four equivalent GaO6 octahedra and corners with three equivalent GaO4 tetrahedra. The corner-sharing octahedra tilt angles range from 55–61°. There is two shorter (1.86 Å) and two longer (1.87 Å) Ga–O bond length. There are four inequivalent O sites. In the first O site, O is bonded in a trigonal planar geometry to three Ga atoms. In the second O site, O is bonded in a trigonal planar geometry to three Ga atoms. In the third O site, O is bonded in a trigonal planar geometry to three Ga atoms. In the fourth O site, O is bonded in a water-like geometry to two Ga atoms.

36 MATERIALS SCIENCE↗

Materials Data on GaO3 by Materials Project

GaO3 is Skutterudite structured and crystallizes in the cubic Im-3 space group. The structure is three-dimensional. Ga is bonded to six equivalent O atoms to form corner-sharing GaO6 octahedra. The corner-sharing octahedral tilt angles are 56°. All Ga–O bond lengths are 1.99 Å. O is bonded in a bent 120 degrees geometry to two equivalent Ga atoms.

36 MATERIALS SCIENCE↗

Materials Data on GaO2 by Materials Project

GaO2 is Hydrophilite-like structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Ga is bonded to six O atoms to form a mixture of corner and edge-sharing GaO6 octahedra. The corner-sharing octahedral tilt angles are 58°. There are a spread of Ga–O bond distances ranging from 1.98–2.04 Å. There are two inequivalent O sites. In the first O site, O is bonded in a trigonal planar geometry to three equivalent Ga atoms. In the second O site, O is bonded in a trigonal non-coplanar geometry to three equivalent Ga atoms.

36 MATERIALS SCIENCE↗