Abstract
Specific-heat measurements on ${\mathrm{K}}_{2}$Os${\mathrm{Cl}}_{6}$ single crystals revealed anomalous behavior at low temperatures. The specific heat of the acoustic modes corresponds to a Debye temperature ${\ensuremath{\Theta}}_{D}$ of 63.6 \ifmmode\pm\else\textpm\fi{} 0.2 K. The contribution of low-lying optical modes including a rotary mode extend the description of the specific heat by the cubic law up to $\frac{T}{{\ensuremath{\Theta}}_{D}}\ensuremath{\simeq}\frac{1}{6}$. A small anomaly of unknown origin occurs, however, at $T=6.67\ifmmode\pm\else\textpm\fi{}0.05$ K. The specific heat and entropy of ${\mathrm{K}}_{2}$Re${\mathrm{Cl}}_{6}$ and ${\mathrm{K}}_{2}$Os${\mathrm{Cl}}_{6}$ evaluated using the technique of the special points in the Brillouin zone agree well with experimental values outside of the regions of structural phase transitions at 103.4 and 110.9 K in ${\mathrm{K}}_{2}$Re${\mathrm{Cl}}_{6}$ and 46.1 K in ${\mathrm{K}}_{2}$Os${\mathrm{Cl}}_{6}$. These calculations permit the evaluation of excess entropies and specific-heat discontinuities associated with the transitions. The critical behavior around the structural phase transition at 46.1 \ifmmode\pm\else\textpm\fi{} 0.5 K in ${\mathrm{K}}_{2}$Os${\mathrm{Cl}}_{6}$ is also discussed. It is concluded that the range of the interaction associated with the transition is approximately the interoctahedral separation.
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