Superposition model for sixfold-coordinated Cr3+ in oxide crystals (EPR study)

The effect of uniaxial (100), (111) and (110) stresses on the EPR fine-structure lines of Cr3+ on octahedral Ti4+ sites in SrTiO3 and Mg2+ sites in MgO have been measured at 300K. The spin-lattice strain coefficients G11 and G44 were determined. From them, the authors deduced the intrinsic superposition-model parameters b2=2.37+or-0.04 cm-1 and t2=-0.36+or-0.01 in SrTiO3, and b2=2.34+or-0.01 cm-1 and t2=-0.12+or-0.11 in MgO, respectively. A substantial dependence of G11 strain coefficients on charge misfit between Cr3+ and the substituted ion was found as has been calculated theoretically by Sangster (1981). The small negative t2 exponents and positive b2 reported here are interpreted as resulting from the three occupied t2g orbitals of the 4A2g ground state of Cr3+ as compared with the 6A1g of Fe3+. A consistent analysis yields a maximum of the positive b2(R) of Cr3+ at Rmax=2.102+or-0.005 AA in MgO, whereas the negative b2(R) of Fe3+ has a minimum at Rmin=1.7+or-0.2 AA. The deduced b2(R) dependence is confirmed for trigonal LaAlO3 and Al2O3, where the known b20(Fe3+)/b20(Cr3+) ratio and sign are quantitatively accounted for.

[1]  J. Clare,et al.  Superposition-model analysis of the spin-strain coupling tensor in ruby , 1983 .

[2]  J. García-solé,et al.  Divalent manganese in an axial symmetry site of additively coloured CaO single crystals , 1983 .

[3]  D. Newman Superposition model analysis of spin Hamiltonian parameters , 1982 .

[4]  J. Krebs,et al.  Confirmation of the EPR identification of Cr 4 + 3 d 2 in p -type Cr-doped GaAs by means of applied uniaxial stress , 1982 .

[5]  S. Misra,et al.  Point-charge and induced-dipole model analysis of spin-Hamiltonian parameters forGd3+doping single crystals of rare-earth-metal trichloride hexahydrates , 1982 .

[6]  Y. Akishige,et al.  ESR Study of Fe3+ in Sr2Nb2O7 at 250°C , 1981 .

[7]  M. Sangster Relaxations and their strain derivatives around impurity ions in MgO , 1981 .

[8]  G. Lehmann,et al.  Correlation of zero-field splittings and site distortions: Variation of b2 FOR Mn2+ with ligand and coordination number , 1981 .

[9]  E. Siegel,et al.  Local position of Fe 3+ in ferroelectric BaTiO 3 , 1979 .

[10]  K. A. Müller,et al.  Structure of transition-metal—oxygen-vacancy pair centers , 1979 .

[11]  W. Berlinger,et al.  Two multipurpose EPR cavities for applications between 1.6 and 1300 K , 1977 .

[12]  J. Andriessen,et al.  EPR ofGd3+-metal-ion complexes in CaF2, BaF2, and SrCl2 , 1977 .

[13]  D. Newman,et al.  Superposition model analysis of Fe3+ and Mn2+ spin-Hamiltonian parameters , 1976 .

[14]  D. Newman,et al.  Interpretation of S-state ion E.P.R. spectra , 1975 .

[15]  D. Newman,et al.  CORRIGENDUM: Analysis of the spin-lattice parameters for Gd3+ and Eu2+ in cubic crystals , 1974 .

[16]  G. Pake,et al.  The physical principles of electron paramagnetic resonance , 1973 .

[17]  W. Berlinger,et al.  Observation of Two Charged States of a Nickel-Oxygen Vacancy Pair in SrTiO3by Paramagnetic Resonance , 1969 .

[18]  E. Feher Effect of Uniaxial Stresses on the Paramagnetic Spectra ofMn3+andFe3+in MgO , 1964 .

[19]  K. Müller,et al.  Nuclear magnetic resonance of La139 and Al27 and electron paramagnetic resonance of Fe3+ in lanthanum aluminate ☆ , 1964 .

[20]  G. Rupprecht,et al.  THE ELASTIC CONSTANTS OF STRONTIUM TITANATE , 1963 .

[21]  G. Bogle,et al.  On the Exactness of the Spin-Hamiltonian Description of Fe3+ in Sapphire , 1962 .

[22]  M. Peter,et al.  Effect of Configuration Mixing and Covalency on the Energy Spectrum of Ruby , 1961 .

[23]  J. Geusic Paramagnetic Fine Structure Spectrum of Cr +++ in a Single Ruby Crystal , 1956 .