STRUCTURE AND ORDERING OF MIXED GARNETS Y3-xRexAl5O12, Re = Er, Yb, Dy

N.A.Grigorieva1, E.V.Charnaya1, V.S.Kasperovich1, S.N.Ivanov2, E.N.Khazanov2

1.Institute of Physics, St.Petersburg State University, Ulyanovskaya 1, Petrodvorets, 198904 St.Petersburg, Russia.
2Institute of Radio Engineering and Electronics, Russian Academy of Sciences, Moscow, Russia.
E-mail:
kasper@snoopy.niif.spb.su

 

A study of the structural order in mixed dielectrics crystals is an actual problem for solid state physics and crystallography.

We present the results of NMR investigation of 27Al in mixed Y3-xRexAl5O12 crystals with concentration x from 0 up to 3, and Re = Er, Yb, Dy. An unit cell of the garnet Y3-xRexAl5O12 contain 40 aluminum ions, 16 of which are situated in an octahedral environment (a-sites), and the other 24 ions in a tetrahedral (d-sites) environment of oxygen ions [1]. The measurements were carried out on an RYa-2301 stationary NMR spectrometer in magnetic fields of 0.5-1T at temperatures of 290K and 77K.

We have calculated the quadrupole interaction parameters e2qQ / h for a- and d-sites from the angular dependence of the NMR spectrum. For both sites in samples of Y3-xErxAl5O12 the quadrupole parameters are left invariant upon the introduction of erbium ions into the lattice, and they are equal to the values e2qQ/h(a) = 0.628 MHz and e2qQ/h(d) = 6.018 MHz. Hence, the substitution of erbium ions for yttrium ions has a minor influence on the structure and chemical composition. For samples Y3-xYbxAl5O12 garnet the values e2qQ/h(a) and e2qQ/h(d) increase linearly from 0.630 MHz up to 1.05 MHz and from 6.02 MHz up to 6.30 MHz, respectively, as content x increases. As to Y3-xDyxAl5O12 the values e2qQ/h(a) and e2qQ/h(d) decrease linearly from 0.630 MHz up to 0.447 MHz and from 6.020 MHz up to 5.873 MHz, respectively, with increasing the concentration x.

Also we have determined the average magnetic moment <m> of the Er ions (6.35 ... 10-25 J/T) and Yb ions (0.83 ... 10-25 J/T) in the garnet lattice from the paramagnetic shift at the room temperature and magnetic field 1T. Note that the obtained value of <m> for the Er ions coincides with magnetic moment of free ion, while one for Yb ions is significantly smaller than <m> of free ion.

We have shown also that crystals Y3-xErxAl5O12 and Y3-xDyxAl5O12 are disordering solid solution for all investigated concentrations x while mixed Y3-xYbxAl5O12 garnets in the range x in [0.75 - 1.00] have an ordered structure. So, the analysis of NMR spectra allows one to determine the character of the substitution ordering in aluminum -yttrium - ytterbium garnets.

1. J.Menzer, Fur Crystallografic, 69 (1928) 300.