A nonlinear susceptibilities (the third derivative of a magnetization mS by a magnetic field h ) of the S=1/2 ferromagnetic Heisenberg chain and the classical Heisenberg chain are calculated at low temperatures $T.$ In both chains the nonlinear susceptibilities diverge as T⁻⁶ and a linear susceptibilities diverge as T⁻². The arbitrary spin S Heisenberg ferromagnet $[$ H = ∑ᵢ₌₁N \ - J Sᵢ Sᵢ₊₁ - (h/S) Sᵢᶻ \ $(J>0),$ $]$ has a scaling relation between mS, h and $T:$ mS(T,h) = F( S² Jh/T²). The scaling function $F(x)$=(2x/3)-(44x³/135) + O(x⁵) is common to all values of spin $S.$
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Nakamura et al. (1994) studied this question.
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