We have proposed an exactly solvable spin-1/2 model defined on 2D decorated lattices of two types. The ground-state phase diagram of the system includes different topological phases with gapless chiral edge states. We show that two types of chiral spin liquid with gapless edge modes are realized on lattices with different symmetry. The phase transition between the topological phase with chiral gapped (Chern number zero) and the topological phase with chiral gapless edge modes (Chern number +/- 1) occurs in the model on the square (symmetric) decorated lattice. On the rectangular (asymmetric) decorated lattice the topological phase is defined by a chiral gapless (gapped) edge mode in the x (y) direction and a chiral gapped (gapless) edge mode in another y (x) direction. We show that a spin-1/2 Kitaev model on a decorated asymmetric square lattice exhibits the quantum phase transition between topological phases with equal Chern numbers. Copyright (C) EPLA, 2013
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Shanghai Qi Zhi Inst, Shanghai 200232, Peoples R China
Tsinghua Univ, Ctr Quantum Informat, IIIS, Beijing, Peoples R ChinaShanghai Qi Zhi Inst, Shanghai 200232, Peoples R China
Dai, Ning
Li, Kai
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Tsinghua Univ, Ctr Quantum Informat, IIIS, Beijing, Peoples R ChinaShanghai Qi Zhi Inst, Shanghai 200232, Peoples R China
Li, Kai
Yang, Yan-Bin
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Tsinghua Univ, Ctr Quantum Informat, IIIS, Beijing, Peoples R China
Hong Kong Univ Sci & Technol, Dept Phys, Clear Water Bay, Hong Kong 999077, Peoples R ChinaShanghai Qi Zhi Inst, Shanghai 200232, Peoples R China
Yang, Yan-Bin
Xu, Yong
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Shanghai Qi Zhi Inst, Shanghai 200232, Peoples R China
Tsinghua Univ, Ctr Quantum Informat, IIIS, Beijing, Peoples R ChinaShanghai Qi Zhi Inst, Shanghai 200232, Peoples R China
机构:
Peking Univ, Sch Phys, State Key Lab Mesoscop Phys, Beijing 100871, Peoples R ChinaPeking Univ, Sch Phys, State Key Lab Mesoscop Phys, Beijing 100871, Peoples R China
Qiao, Hong
Sun, Zheng-Hang
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Chinese Acad Sci, Inst Phys, Beijing 100190, Peoples R China
Univ Chinese Acad Sci, Sch Phys Sci, Beijing 100190, Peoples R ChinaPeking Univ, Sch Phys, State Key Lab Mesoscop Phys, Beijing 100871, Peoples R China
Sun, Zheng-Hang
Sun, Feng-Xiao
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Peking Univ, Sch Phys, State Key Lab Mesoscop Phys, Beijing 100871, Peoples R China
Collaborat Innovat Ctr Quantum Matter, Beijing, Peoples R ChinaPeking Univ, Sch Phys, State Key Lab Mesoscop Phys, Beijing 100871, Peoples R China
Sun, Feng-Xiao
Mu, Liang-Zhu
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Peking Univ, Sch Phys, Beijing 100871, Peoples R ChinaPeking Univ, Sch Phys, State Key Lab Mesoscop Phys, Beijing 100871, Peoples R China
Mu, Liang-Zhu
He, Qiongyi
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Peking Univ, Sch Phys, State Key Lab Mesoscop Phys, Beijing 100871, Peoples R China
Collaborat Innovat Ctr Quantum Matter, Beijing, Peoples R China
Shanxi Univ, Collaborat Innovat Ctr Extreme Opt, Taiyuan 030006, Shanxi, Peoples R China
Beijing Acad Quantum Informat Sci, Beijing 100193, Peoples R ChinaPeking Univ, Sch Phys, State Key Lab Mesoscop Phys, Beijing 100871, Peoples R China
He, Qiongyi
Fan, Heng
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机构:
Chinese Acad Sci, Inst Phys, Beijing 100190, Peoples R China
Univ Chinese Acad Sci, Sch Phys Sci, Beijing 100190, Peoples R China
Collaborat Innovat Ctr Quantum Matter, Beijing, Peoples R China
Beijing Acad Quantum Informat Sci, Beijing 100193, Peoples R China
CAS Cent Excellence Topol Quantum Computat, Beijing 100190, Peoples R ChinaPeking Univ, Sch Phys, State Key Lab Mesoscop Phys, Beijing 100871, Peoples R China