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Heat-capacity measurements have been made on pure palladium and a series of dilute palladium-iron alloys over the temperature range 1.4 to 100^∘{}K. All alloys exhibit a ferromagnetic specific heat anomaly, the entropy of which is proportional to iron concentration. This entropy corresponds to a mean spin of 1.1±{}0.3 per iron atom. The disagreement between the latter figure and the value obtained from the saturation moment of more concentrated alloys is discussed. For the most concentrated alloy a T3/2 spin-wave term is observed, the magnitude of which is in approximate agreement with theory. The Debye θ for pure palladium appears to have an anomalous temperature dependence.
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Veal et al. (1964) studied this question.
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