首页> 外文期刊>Physical Review, B. Condensed Matter >From the square lattice to the checkerboard lattice: Spin-wave and large-n limit analysis - art. no. 184408
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From the square lattice to the checkerboard lattice: Spin-wave and large-n limit analysis - art. no. 184408

机译:从方格到棋盘格:自旋波和大n极限分析-艺术。没有。 184408

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摘要

Within a spin wave analysis and a fermionic large-n limit, it is shown that the antiferromagnetic Heisenberg model on the checkerboard lattice may have different ground states, depending on the spin size S. Through an additional exchange interaction that corresponds to an intertetrahedra coupling, the stability of the Neel state has been explored for all cases from the square lattice to the isotropic checkerboard lattice. Away from the isotropic limit and within the linear spin-wave approximation, it is shown that there exists a critical coupling for which the local magnetization of the Neel state vanishes for any value of the spin S. One the other hand, using the Dyson-Maleev approximation, this result is valid only in the case S=1/2 and the limit between a stable and an unstable Neel state is at S=1. For S=1/2, the fermionic large-n limit suggests that the ground state is a valence-bond solid build with disconnected four-spin singlets. This analysis indicates that for low spin and in the isotropic limit, the checkerboard antiferromagnet may be close to an instability between an ordered S=0 ground state and a magnetized ground state. [References: 39]
机译:在自旋波分析和费米电子大n限内,表明棋盘格上的反铁磁Heisenberg模型可能具有不同的基态,具体取决于自旋大小S。通过与四面体耦合相对应的附加交换相互作用,从方格到各向同性的棋盘格,都探索了Neel态的稳定性。远离各向同性极限并在线性自旋波近似值内,表明存在一个临界耦合,对于该耦合,Ne态的局部磁化强度对于自旋S的任何值均消失。另一方面,使用Dyson- Maleev近似,此结果仅在S = 1/2且稳定Neel状态和不稳定Neel状态之间的界限为S = 1的情况下才有效。对于S = 1/2,费米离子的大n限表明基态是具有断开的四旋线单重态的价键固体结构。该分析表明,对于低自旋和各向同性极限,棋盘状反铁磁体可能接近有序S = 0基态和磁化基态之间的不稳定性。 [参考:39]

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