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Fermionic Symmetry Protected Topological Phase Induced by Interaction Shangqiang NING First year PHD student Institute For Advanced Study, Tsinghua University Email: nsq12382@126.com
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Collaborators Hongchen Jiang Slac, Stanford Zhengxin Liu IASTU, Beijing
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Outline 1. Background and motivation 2. Study of a specific model 3. Conclusion
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Background and Motivation 2D topological insulator Key properties of TI: Band insulator Mass terms breaks T breaks U(1) X. Qi, S.C. Zhang RevModPhys.83.1057
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Symmetry Protected Topological phase (SPT phase) gapped gapless
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Classification of SPT For more symmetry group in
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∎ SPT phases also exist in Bosonic systems S=1 Haldane phase (Bosonic) Finite excitation gap No symmetry breaking SO(3) symmetry protected spin-1/2 edge states Degeneracy of entanglement spectrum Spin-1/2 Spin-1 Haldane 83; Affleck, Kennedy, Lieb, Tasaki 87 Gu, Wen 09; Pollmann et.al 09; Chen,Gu,Wen 11 bulk gap SO(3) symmetry
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A B
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Entanglement spectrum J 2 /J 1 =0.9 SO(3) symmetry Non trivial Trivial
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Classification of Bosonic SPT SO(3) symmetry : 2 phases Xie Chen, Zheng-Cheng Gu, and Xiao-Gang Wen,2011
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Classification of Interacting Fermionic SPT 1D superconductor 2D superconductor Time reversal and mirror reflect ZZ8Z8 It seems that interactions reduce the classification. However, it maybe not true! Hong Yao and Shinsei Ryu, arXiv :1202.5805 Evelyn Tang and Xiao-Gang Wen arXiv:1204.0520v2
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Model
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Symmetry and classification free case, only the trivial phase. 2 projective representation two SPT phases.
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Non-interacting limit U=0, J=0 = 2-fold
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Non-interacting limit U=0, J=0 SPT only focus on gapped phases. Open boundary, no zero mode, indicating the trivialness of phase
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Add Hubbard interaction the band insulator and the Mott insulator are adiabatically connected
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Interacting case
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Competition
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Interacting case
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We find two phases in the interacting case : trivial insulator and Haldane insulator
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Conclusion
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Thanks for your attention!
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