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arXiv 1809.04895cond-mat.stat-mech
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双修饰蜂窝晶格上自旋-电子耦合模型中重入相变的涨落

Rise and Fall of Reentrant Phase Transitions in a Coupled Spin-Electron Model on a Doubly Decorated Honeycomb Lattice

Hana Čenčariková, Jozef Strečka

摘要:

严格计算了双装饰蜂窝晶格上自旋-电子耦合模型的相图和自发磁化强度,该模型考虑了移动电子在装饰位上的量子力学跳跃、移动电子与局域自旋之间的最近邻伊辛耦合以及节点位上局域自旋之间的远邻伊辛耦合.自发有序的铁磁相,自发有序的反铁磁相和无序的顺磁相出现在相图中取决于装饰网站的电子填充,跳跃项的相对大小和都考虑耦合常数。它是证明的性质和大小的进一步邻居伊辛耦合之间的本地化自旋基本上影响的上升和下降的再入过渡接近的顺磁相和两个自发有序相之间的相边界。

英文摘要:

Phase diagrams and spontaneous magnetization are rigorously calculated for a coupled spin-electron model on a doubly decorated honeycomb lattice, which accounts for a quantum-mechanical hopping of the mobile electrons on decorating sites, the nearest-neighbor Ising coupling between mobile electrons and localized spins, as well as, the further-neighbor Ising coupling between the localized spins placed on nodal sites. The spontaneously ordered ferromagnetic phase, spontaneously ordered antiferromagnetic phase and disordered paramagnetic phase emerge in a phase diagram depending on an electron filling of the decorating sites, a relative size of the hopping term and both considered coupling constants. It is evidenced that a nature and size of the further-neighbor Ising coupling between the localized spins basically influences rise and fall of reentrant transitions close to a phase boundary between the paramagnetic phase and both spontaneously ordered phases.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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