Publication | Open Access
Comparison of <scp>EPR</scp> spectra of the Gd<sup>3+</sup> ion‐doped <scp>YA</scp>l<sub>3</sub>(<scp>BO</scp><sub>3</sub>)<sub>4</sub>, Eu<scp>A</scp>l<sub>3</sub>(<scp>BO</scp><sub>3</sub>)<sub>4</sub>, and Tm<scp>A</scp>l<sub>3</sub>(<scp>BO</scp><sub>3</sub>)<sub>4</sub> single crystals
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Citations
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References
2013
Year
Rare Earth MineralCrystal StructureEngineeringSolid-state ChemistryImpurity Gd 3+ChemistrySpectroscopic PropertySpectra-structure CorrelationQuantum MaterialsPhysicsCrystal MaterialAluminum BoratesQuantum ChemistryCrystallographySolid-state PhysicCrystal Structure DesignNatural SciencesSpectroscopyCondensed Matter PhysicsApplied PhysicsIsomorphic Aluminum Borates
The EPR spectra of Gd 3+ ion replacing Y 3+ or rare‐earth (RE) ions in aluminum borates REAl 3 (BO 3 ) 4 (RE = Y 3+ , Eu 3+ , Tm 3+ ) have been studied. The spin‐Hamiltonian parameters of an impurity Gd 3+ ion in these crystals were determined. The basic atom coordinates in the structure of TmAl 3 (BO 3 ) 4 crystal have been established. Distortions of the Gd 3+ ion nearest environment were analyzed within the framework of the superposition model of zero‐field splitting. The parameter change in isomorphic aluminum borates is shown to be determined by change of the angle between the Gd 3+ O 2− bond and the C 3 ‐axis.
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