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Superposition model for sixfold-coordinated Cr<sup>3+</sup>in oxide crystals (EPR study)
86
Citations
12
References
1983
Year
Materials ScienceTransition Metal ChalcogenidesEngineeringInorganic MaterialNatural SciencesSubstituted IonApplied PhysicsCondensed Matter PhysicsStrain CoefficientsQuantum ChemistryChemistrySrtio 3Electronic StructureCrystallographyCrystal Structure DesignSuperposition Model
The effect of uniaxial (100), (111) and (110) stresses on the EPR fine-structure lines of Cr 3+ on octahedral Ti 4+ sites in SrTiO 3 and Mg 2+ sites in MgO have been measured at 300K. The spin-lattice strain coefficients G 11 and G 44 were determined. From them, the authors deduced the intrinsic superposition-model parameters b 2 =2.37+or-0.04 cm -1 and t 2 =-0.36+or-0.01 in SrTiO 3 , and b 2 =2.34+or-0.01 cm -1 and t 2 =-0.12+or-0.11 in MgO, respectively. A substantial dependence of G 11 strain coefficients on charge misfit between Cr 3+ and the substituted ion was found as has been calculated theoretically by Sangster (1981). The small negative t 2 exponents and positive b 2 reported here are interpreted as resulting from the three occupied t 2g orbitals of the 4 A 2g ground state of Cr 3+ as compared with the 6 A 1g of Fe 3+ . A consistent analysis yields a maximum of the positive b 2 (R) of Cr 3+ at R max =2.102+or-0.005 AA in MgO, whereas the negative b 2 (R) of Fe 3+ has a minimum at R min =1.7+or-0.2 AA. The deduced b 2 (R) dependence is confirmed for trigonal LaAlO 3 and Al 2 O 3 , where the known b 2 0 (Fe 3+ )/b 2 0 (Cr 3+ ) ratio and sign are quantitatively accounted for.
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