SrF2 and BaF2 crystals, doped
with the Yb3+
ions, have been investigated by electron paramagnetic resonance
and optical spectroscopy. As-grown crystals of SrF2 and
BaF2
show the two paramagnetic centres for the cubic (Tc) and trigonal (T4) symmetries of
the Yb3+
ions. Empirical diagrams of the energy levels were established and the potentials
of the crystal field were determined. Information was obtained on the SrF2 and
BaF2
phonon spectra from the electron-vibrational structure of the optical
spectra. The crystal field parameters were used to analyse the crystal
lattice distortions in the vicinity of the impurity ion and the F−
ion compensating for the excess positive charge in T4.
Within the frames of a superposition model, it is shown that three F− ions
from the nearest surrounding cube, located symmetrically with respect to the C3
axis from the side of the ion-compensator, approach the impurity
ion and cling to the axis of the centre when forming T4. The
F−
ion located on the axis of the centre between the Yb3+
ion and ion-compensator, also approaches close to the impurity ion.
Electron paramagnetic resonance, electron-nuclear double resonance, and optical spectroscopy of the tetragonal Yb 3ϩ center in KMgF 3 are reported here. The results of these experiments allow us to conclude that a previously given structural model as well as the interpretation of the optical spectrum of this center are incorrect. A model is presented and experimentally and theoretically justified. In particular, the values of the hyperfine and transferred hyperfine interaction parameters were determined as well as an experiment-based energy-level scheme. Its parametrization is performed by including simultaneously the crystal field and the spin-orbit interaction within the 7 F term. Furthermore, a theoretical analysis of the transferred hyperfine interaction ͑THFl͒ parameters is presented. It is further shown from optics and from microscopic calculations of the THFI parameters that g ʈ and g Ќ have opposite signs and that the rule of correspondence between the cubic g factor and g ϭ 1 3 (g x ϩg y ϩg z) does not depend on the relative magnitude of the cubic and lowsymmetry crystal field acting on the rare-earth ion.
The Yb 3+ paramagnetic center of the trigonal symmetry (''oxygen'' paramagnetic center T 2 ) in CaF 2 and SrF 2 single crystals is studied by EPR and optical spectroscopy. The Stark level energies of the Yb 3+ multiplets are established from absorption, luminescence and excitation luminescence spectra and the crystal field parameters are calculated. r
In Table I, we made a typo: instead of A || ( 163 Dy) = 300.8×10 −4 cm −1 ; A ⊥ ( 163 Dy) = 236.8×10 −4 cm −1 , one should read A || ( 163 Dy) = 236.8×10 −4 cm −1 ; A ⊥ ( 163 Dy) = 300.8×10 −4 cm −1 . 2469-9950/2016/94(7)/079902 (1) 079902-1
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