Heisenberg-Kitaev model on the hyperhoneycomb lattice

被引:87
|
作者
Lee, Eric Kin-Ho [1 ,2 ]
Schaffer, Robert [1 ,2 ]
Bhattacharjee, Subhro [1 ,2 ]
Kim, Yong Baek [1 ,2 ,3 ]
机构
[1] Univ Toronto, Dept Phys, Toronto, ON M5S 1A7, Canada
[2] Univ Toronto, Ctr Quantum Mat, Toronto, ON M5S 1A7, Canada
[3] Korea Inst Adv Study, Sch Phys, Seoul 130722, South Korea
来源
PHYSICAL REVIEW B | 2014年 / 89卷 / 04期
基金
加拿大自然科学与工程研究理事会;
关键词
TOPOLOGICAL INSULATORS; PHASE; BAND;
D O I
10.1103/PhysRevB.89.045117
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Motivated by recent experiments on beta-Li2IrO3, we study the phase diagram of the Heisenberg-Kitaev model on a three-dimensional lattice of tricoordinated Ir4+, dubbed the hyperhoneycomb lattice. The lattice geometry of this material, along with Ir4+ ions carrying J(eff) = 1/2 moments, suggests that the Heisenberg-Kitaev model may effectively capture the low-energy spin-physics of the system in the strong-coupling limit. Using a combination of semiclassical analysis, exact solution, and slave-fermion mean-field theory, we find, in addition to the spin liquid, four different magnetically ordered phases depending on the parameter regime. All four magnetic phases-the Neel, the polarized ferromagnet, the skew-stripy, and the skew-zig-zag-have collinear spin ordering. The three-dimensional Z(2) spin liquid, which extends over an extended parameter regime around the exactly solvable Kitaev point, has a gapless Majorana mode with a deformed Fermi circle (codimensions, d(c) = 2). We discuss the effect of the magnetic field and finite temperature on different phases that may be relevant for future experiments.
引用
收藏
页数:13
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