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Complexes of Several Spins in a Linear Heisenberg Chain

А. А. Овчинников

Published Jan 1, 1967• 4 citations
OpenAlex

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The Free Energy and the Scaling Function of the Ferromagnetic Heisenberg Chain in a Magnetic Field

Hiroaki Nakamura, Minoru Takahashi

A nonlinear susceptibilities (the third derivative of a magnetization $m_S$ 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 $[$ ${\cal H} = \sum_{i=1}^{N} \{ - J{\bf S}_{i} {\bf S}_{i+1} - (h/S) S_{i}^{z} \}$ $(J>0),$ $]$ has a scaling relation between $m_S,$ $h$ and $T:$ $m_S(T,h) = F( S^2 Jh/T^2).$ The scaling function $F(x)$=(2$x$/3)-(44$x^{3}$/135) + O($x^{5}$) is common to all values of spin $S.$

arXiv:cond-mat/9401074•Journal of the Physical Society of Japan•Jul 15, 1994•20 citations
A nonlinear susceptibilities (the third derivative of a magnetization mSm_SmS​ by a magnetic field hhh ) of the SSS=1/2 ferromagnetic Heisenberg chain and the classical Heisenberg chain are calculated at low temperatures T.T.T. In both chains the nonlinear susceptibilities diverge as T−6T^{-6}T−6 and a linear susceptibilities diverge as T−2.T^{-2}.T−2. The arbitrary spin SSS Heisenberg ferromagnet [[[ H=∑i=1N{−JSiSi+1−(h/S)Siz}{\cal H} = \sum_{i=1}^{N} \{ - J{\bf S}_{i} {\bf S}_{i+1} - (h/S) S_{i}^{z} \}H=∑i=1N​{−JSi​Si+1​−(h/S)Siz​} (J>0),(J>0),(J>0), ]]] has a scaling relation between mS,m_S,mS​, hhh and T:T:T: mS(T,h)=F(S2Jh/T2).m_S(T,h) = F( S^2 Jh/T^2).mS​(T,h)=F(S2Jh/T2). The scaling function F(x)F(x)F(x)=(2xxx/3)-(44x3x^{3}x3/135) + O(x5x^{5}x5) is common to all values of spin S.S.S.