Abstract

Temperature dependence of spontaneous magnetization, ${M}_{s}(T)$, corresponding to the single-domain ferromagnetic state, has been studied experimentally using high-purity single crystals of Gd, Tb, and Dy. The resulting ${M}_{s}(T)$ curves follow the ``$3∕2\ensuremath{-}5∕2\ensuremath{-}1∕3$ law.'' Anomalies due to the crystal-field gap and to the helix-ferromagnet transition in Tb and Dy are practically indiscernible.

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