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Spin-$1$ $J_1-J_2-J_3$ ferromagnetic Heisenberg model with an easy-plane crystal field on the cubic lattice: A bosonic approach

机译:旋转 - $ 1 $ $ J_1-J_2-J_3 $铁磁海森堡模型,具有简易平面   立方晶格上的晶场:一种玻色子方法

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摘要

We examine the phase diagram of the spin-$1$ $J_1-J_2-J_3$ ferromagneticHeisenberg model with an easy-plane crystal field on the cubic lattice, inwhich $J_1$ is the ferromagnetic exchange interaction between nearestneighbors, $J_2$ is the antiferromagnetic exchange interaction betweennext-nearest neighbors and $J_3$ is the antiferromagnetic exchange interactionbetween next-next-nearest neighbors. Using the bond-operator formalism, weinvestigate the phase transitions between the disordered paramagnetic phase andthe ordered ones. We show that the nature of the quantum phase transitions change as thefrustration parameters ($\frac{J_2}{J_1}$, $\frac{J_3}{J_1}$) are varied. Thezero-temperature phase diagram exhibits second- and first-order transitions,depending on the energy gap behavior. Remarkably, we find a disorderednonmagnetic phase, even in the absence of a crystal field, which is suggestedto be a quantum spin liquid candidate. We also depict the phase diagram atfinite temperature for some values of crystal field and frustration parameters.
机译:我们检查自旋$ 1 $ $ J_1-J_2-J_3 $铁磁的相图在立方晶格上具有易平面晶体场的海森堡模型,其中$ J_1 $是最近邻之间的铁磁交换相互作用,$ J_2 $是反铁磁近邻与$ J_3 $之间的交换相互作用是近邻与近邻之间的反铁磁交换相互作用。利用键合形式论,研究了无序顺磁相与有序顺磁相之间的相变。我们显示出量子相变的性质随挫折参数($ \ frac {J_2} {J_1} $,$ \ frac {J_3} {J_1} $)的变化而变化。零温度相图显示出二阶和一阶跃迁,具体取决于能隙行为。值得注意的是,即使在没有晶体场的情况下,我们也发现了无序的非磁性相,这被认为是量子自旋液体的候选物。我们还描述了在某些温度下的某些晶场值和无奈参数的相图。

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