Abstract

The heat capacities of the compounds DyAl 2, ErAl 2 and LuAl 2 were measured in an adiabatic calorimeter from approximately 5 to 300 K. The compounds DyAl 2 and ErAl 2 show C P anomalies at 58.0 and 10.2 K, respectively, which are attributed to the destruction of magnetic order. In order to separate the crystal field and magnetic contributions from the measured heat capacities, it was necessary to evaluate the lattice heat capacity. The lattice term, C L was obtained from the C P data of LuAl 2 by a method of interpolation which gave values of C L for an arbitrary R Al 2 compound. Using this “interpolated lattice blank”, excess entropies associated with the crystal field and magnetic terms were computed throughout the series. These values are quite close to R In (2 J + 1). The results also indicate that, for the compounds studied, the degeneracy of the lowest ground state is completely lifted. In addition, the magnetic contribution to the heat capacity of the magnetically ordered R A1 2 phases was found to exhibit an exponential dependence below the temperature corresponding to the spin wave energy gap and a T 3 2 dependence above this temperature. Detailed calculations were performed to characterize the influence of cubic crystal field in ErAl 2 on the 4 I 15 2 ground state multiplet of the Er 3+ ion. It is concluded that the magnetic ordering in ErAl 2 takes place within the Γ 8 3 quartet state. Smoothed values of heat capacity, entropy and related thermodynamic functions are tabulated.

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