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• W2012894906 abstract "We study a spin model on honeycomb lattice with two types of Heisenberg exchange couplings, $J$ and $stackrel{ifmmode tilde{}else ~{}fi{}}{J}$, where $J$ is for the conventional spin and $stackrel{ifmmode tilde{}else ~{}fi{}}{J}$ is for rotated spin. When $J=0$, the system is either in a stripy antiferromagnetic order ($stackrel{ifmmode tilde{}else ~{}fi{}}{J}<0$, ferromagnetic for rotated spin) or a zigzag antiferromagnetic order ($stackrel{ifmmode tilde{}else ~{}fi{}}{J}>0$, antiferromagnetic for rotated spin). The competition between two ferromagnetic orders or between two antiferromagnetic orders induces Kitaev's spin liquid phase, characterized by the exactly solvable Kitaev model ($J=stackrel{ifmmode tilde{}else ~{}fi{}}{J}$). Our model can be applied to layered Mott insulators $A$${}_{2}$IrO${}_{3}$ ($A=text{Li}$, Na). For a monolayer of Li${}_{2}$IrO${}_{3}$, we show that it is possible to tune the controlling parameter into the Kitaev spin liquid regime by a link-dependent Rashba spin-orbital coupling." @default.
• W2012894906 created "2016-06-24" @default.
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• W2012894906 date "2013-01-29" @default.
• W2012894906 modified "2023-10-18" @default.
• W2012894906 title "Tuning into the Kitaev spin liquid phase: A spin model on the honeycomb lattice with two types of Heisenberg exchange couplings" @default.
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• W2012894906 doi "https://doi.org/10.1103/physrevb.87.041107" @default.
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