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Spin-stiffness of anisotropic Heisenberg model on square lattice and possible mechanism for pinning of the electronic liquid crystal direction in YBCO

机译:方形和格子上各向异性海森堡模型的自旋刚度   电子液晶方向钉扎的可能机制   YBCO

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摘要

Using series expansions and spin-wave theory we calculate the spin-stiffnessanisotropy $\rho_{sx}/\rho_{sy}$ in Heisenberg models on the square latticewith anisotropic couplings $J_x,J_y$. We find that for the weakly anisotropicspin-half model ($J_x\approx J_y$), $\rho_{sx}/\rho_{sy}$ deviatessubstantially from the naive estimate $\rho_{sx}/\rho_{sy} \approx J_x/J_y$. Weargue that this deviation can be responsible for pinning the electronic liquidcrystal direction, a novel effect recently discovered in YBCO. Forcompleteness, we also study the spin-stiffness for arbitrary anisotropy$J_x/J_y$ for spin-half and spin-one models. In the limit of $J_y/J_x\to 0$,when the model reduces to weakly coupled chains, the two show dramaticallydifferent behavior. In the spin-one model, the stiffness along the chains goesto zero, implying the onset of Haldane-gap phase, whereas for spin-half thestiffness along the chains increases monotonically from a value of $0.18 J_x$for $J_y/J_x=1$ towards $0.25 J_x$ for $J_y/J_x\to 0$. Spin-wave theory isextremely accurate for spin-one but breaks down for spin-half presumably due tothe onset of topological terms.
机译:使用级数展开和自旋波理论,我们在具有各向异性耦合$ J_x,J_y $的方格上的Heisenberg模型中,计算了海森堡模型中的自旋刚度各向异性$ \ rho_ {sx} / \ rho_ {sy} $。我们发现,对于弱各向异性的半自旋模型($ J_x \ approx J_y $),$ \ rho_ {sx} / \ rho_ {sy} $与天真估计$ \ rho_ {sx} / \ rho_ {sy} \大约J_x / J_y $。担心这种偏离可能是造成电子液晶方向固定的原因,这是YBCO最近发现的一种新颖效果。对于完整性,我们还研究了半自旋模型和自旋一模型的任意各向异性$ J_x / J_y $的自旋刚度。在$ J_y / J_x \限制为0 $的情况下,当模型简化为弱耦合链时,两者表现出截然不同的行为。在自旋模型中,沿链的刚度变为零,这意味着Haldane间隙相的开始,而对于自旋半,沿链的刚度从$ 0.18的值单调增加,J_x $为$ J_y / J_x = 1 $朝$ 0.25 J_x $兑换$ J_y / J_x \至0 $。自旋波理论对于自旋一是极其精确的,但对于自旋半是无效的,大概是由于拓扑项的出现。

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