Crystal growth, structure and crystal field splitting and fitting of Yb:GdScO<sub>3</sub>

Abstract A good quality (5 at.% Yb:GdScO 3 ) single crystal of Φ 30 mm × 37 mm was grown successfully by the Czochralski method. Its structure is studied by the x-ray diffraction (XRD), and its atomic coordinates are obtained by Rietveld refinement. The crystal field energy level splitting of Yb 3+ in GdScO 3 is determined by employing the absorption and photoluminescence spectra at 8 K. Only 2 F 7/2 (4) is far from the ground state 2 F 7/2 (1) by 710 cm −1 among the crystal field energy levels split from 2 F 7/2 , so it is more easier to realize the laser operation of 2 F 5/2 (1)→ 2 F 7/2 (4) with wavelength 1060 nm. The spin–orbit coupling parameters and intrinsic crystal field parameters (CFPs). The intrinsic crystal field parameters <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msub> <mml:mover accent="true"> <mml:mi>B</mml:mi> <mml:mo stretchy="false">¯</mml:mo> </mml:mover> <mml:mi>k</mml:mi> </mml:msub> </mml:mrow> </mml:math> ( k = 2, 4, 6) of the crystal were fitted by the superposition model. The CFPs evaluated with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msub> <mml:mover accent="true"> <mml:mi>B</mml:mi> <mml:mo stretchy="false">¯</mml:mo> </mml:mover> <mml:mi>k</mml:mi> </mml:msub> </mml:mrow> </mml:math> and coordination factor are taken as the initial parameters to fit the crystal field energy levels of the crystal, and the crystal field parameters <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msubsup> <mml:mi>B</mml:mi> <mml:mi>q</mml:mi> <mml:mi>k</mml:mi> </mml:msubsup> </mml:mrow> </mml:math> are obtained finally with the root-mean-square deviation 9 cm −1 . It is suggested that the ligand point charge, covalency and overlap interaction are slightly weaker than charge interpenetration and coulomb exchange interaction for Yb 3+ in GdScO 3 . The obtained Hamiltonian parameters can be used to calculate crystal field energy levels and wave functions of Yb:GdScO 3 to analyze the mechanism of the luminescence or laser.

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Publication Details

Journal
Chinese Physics B
Published
2024-08-23
DOI
https://doi.org/10.1088/1674-1056/ad72d3
Citations
3
Primary Topic
Nuclear materials and radiation effects
Type
article
Field-Weighted Citation Impact
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article

Crystal growth, structure and crystal field splitting and fitting of Yb:GdScO3

Jia-Hong 加红 Li 李, Qing-Li 庆礼 Zhang 张, Gui-Hua 贵花 Sun 孙, Jin-Yun 进云 Gao 高 et al.
3 citations
Chinese Physics B
Nuclear materials and radiation effects
0.35
article

Crystal growth, structure and crystal field splitting and fitting of Yb:GdScO3

Jia-Hong 加红 Li 李, Qing-Li 庆礼 Zhang 张, Gui-Hua 贵花 Sun 孙, Jin-Yun 进云 Gao 高, Ren-Qin 仁勤 Dou 窦, Xiao-Fei 小飞 Wang 王, Shou-Jun 守军 Ding 丁
article en
3 citations

Abstract

Abstract A good quality (5 at.% Yb:GdScO 3 ) single crystal of Φ 30 mm × 37 mm was grown successfully by the Czochralski method. Its structure is studied by the x-ray diffraction (XRD), and its atomic coordinates are obtained by Rietveld refinement. The crystal field energy level splitting of Yb 3+ in GdScO 3 is determined by employing the absorption and photoluminescence spectra at 8 K. Only 2 F 7/2 (4) is far from the ground state 2 F 7/2 (1) by 710 cm −1 among the crystal field energy levels split from 2 F 7/2 , so it is more easier to realize the laser operation of 2 F 5/2 (1)→ 2 F 7/2 (4) with wavelength 1060 nm. The spin–orbit coupling parameters and intrinsic crystal field parameters (CFPs). The intrinsic crystal field parameters <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msub> <mml:mover accent="true"> <mml:mi>B</mml:mi> <mml:mo stretchy="false">¯</mml:mo> </mml:mover> <mml:mi>k</mml:mi> </mml:msub> </mml:mrow> </mml:math> ( k = 2, 4, 6) of the crystal were fitted by the superposition model. The CFPs evaluated with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msub> <mml:mover accent="true"> <mml:mi>B</mml:mi> <mml:mo stretchy="false">¯</mml:mo> </mml:mover> <mml:mi>k</mml:mi> </mml:msub> </mml:mrow> </mml:math> and coordination factor are taken as the initial parameters to fit the crystal field energy levels of the crystal, and the crystal field parameters <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msubsup> <mml:mi>B</mml:mi> <mml:mi>q</mml:mi> <mml:mi>k</mml:mi> </mml:msubsup> </mml:mrow> </mml:math> are obtained finally with the root-mean-square deviation 9 cm −1 . It is suggested that the ligand point charge, covalency and overlap interaction are slightly weaker than charge interpenetration and coulomb exchange interaction for Yb 3+ in GdScO 3 . The obtained Hamiltonian parameters can be used to calculate crystal field energy levels and wave functions of Yb:GdScO 3 to analyze the mechanism of the luminescence or laser.

Chinese Physics BVol. 33(11)
University of Science and Technology of China (CN), Hefei Institutes of Physical Science (CN), Anhui Institute of Optics and Fine Mechanics (CN), Anhui University of Technology (CN)
Affordable and clean energy
Openalex Percentile: Top 45%
Nuclear materials and radiation effects
0.35
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