Abstract
We show that the low-temperature susceptibility of Ce ${(\mathrm{I}\mathrm{n},\phantom{\rule{0ex}{0ex}}\mathrm{S}\mathrm{n})}_{3}$ compounds has a quadratic temperature dependence with positive coefficient. We demonstrate that this behavior is well accounted for by a generalization to arbitrary band shapes of the paramagnon theory, which has been applied previously to liquid $^{3}\mathrm{He}$. This result is relevant to the whole class of mixed-valence materials. We conclude that the previously proposed phenomenology that treats valence-fluctuation materials as heavy, nearly magnetic Fermi liquids finds further support in the present analysis.
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