4.7 Article

Thermodynamic behavior of modified integer-spin Kitaev models on the honeycomb lattice

期刊

PHYSICAL REVIEW E
卷 103, 期 2, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevE.103.022109

关键词

-

资金

  1. U.S. National Science Foundation DMR Grant [1855111]
  2. DST, India [SR/S2/JCB-44/2010]
  3. Direct For Mathematical & Physical Scien [1855111] Funding Source: National Science Foundation
  4. Division Of Materials Research [1855111] Funding Source: National Science Foundation

向作者/读者索取更多资源

This study examines the thermodynamic behavior of modified spin-S Kitaev models, finding distinct properties for half-odd-integer spins and integer spins. Various thermodynamic properties are explored through transfer matrix methods, high-temperature expansions, and Monte Carlo simulations for ferromagnetic and antiferromagnetic models with spin S = 1 and S = 2. The results reveal a range of behaviors, including finite, critical, or exponential correlation lengths as temperature approaches zero, as well as differences in the saturation of Z(2) flux variables among different models.
We study the thermodynamic behavior of modified spin-S Kitaev models introduced by Baskaran, Sen, and Shankar [Phys. Rev. B 78, 115116 (2008)]. These models have the property that for half-odd-integer spins their eigenstates map on to those of spin-1/2 Kitaev models, with well-known highly entangled quantum spin-liquid states and Majorana fermions. For integer spins, the Hamiltonian is made out of commuting local operators. Thus, the eigenstates can be chosen to be completely unentangled between different sites, though with a significant degeneracy for each eigenstate. For half-odd-integer spins, the thermodynamic properties can be related to the spin-1/2 Kitaev models apart from an additional degeneracy. Hence we focus here on the case of integer spins. We use transfer matrix methods, high-temperature expansions, and Monte Carlo simulations to study the thermodynamic properties of ferromagnetic and antiferromagnetic models with spin S = 1 and S = 2. Apart from large residual entropies, which all the models have, we find that they can have a variety of different behaviors. Transfer matrix calculations show that for the different models, the correlation lengths can be finite as T -> 0, become critical as T -> 0, or diverge exponentially as T -> 0. The Z(2) flux variable associated with each hexagonal plaquette saturates at the value +1 as T -> 0 in all models except the S = 1 antiferromagnet where the mean flux remains zero as T -> 0. We provide qualitative explanations for these results.

作者

我是这篇论文的作者
点击您的名字以认领此论文并将其添加到您的个人资料中。

评论

主要评分

4.7
评分不足

次要评分

新颖性
-
重要性
-
科学严谨性
-
评价这篇论文

推荐

暂无数据
暂无数据