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We construct a two-band lattice model whose bands can carry the Chern numbers C=0,pm1,pm2.
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The importance of one-body terms was understood during a discussion between Neupert and Bernevig in 2011 to resolve the apparent paradox that Ref. 23 was finding numerical evidences for a FCI at the filling fraction 2/3 while Bernevig and Regnault in Ref. 24 were not. In effect, Ref. 23 studies H ~ \widetilde{H} while Ref. 24 studies H H at the filling fraction 2/3
2011
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T. Neupert, L. Santos, S. Ryu, C. Chamon, and C. Mudry, Phys. Rev. B 84
2011
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B. A. Bernevig, “Inversion Symmetric Topological Insulators and Fractional Chern Insulator,”
2011
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B. A. Bernevig and N. Regnault, Phys. Rev. B 85
2012
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Y.-F. Wang, H. Yao, Z.-C. Gu, C.-D. Gong, D. N. Sheng, Phys. Rev. Lett. 108
2012
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2008
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T. Neupert, L. Santos, C. Chamon, and C. Mudry, Phys. Rev. Lett. 106
2011
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D. N. Sheng, Z. Gu, K. Sun, and L. Sheng, Nature Communications 2
2011
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Y.-F. Wang, Z.-C. Gu, C.-D. Gong, D. N. Sheng, Phys. Rev. Lett. 107
2011
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N. Regnault and B. A. Bernevig, Phys. Rev. X 1
2011
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T. Liu, C. Repellin, B. A. Bernevig, and N. Regnault, arXiv:1206.2626 (unpublished)
Cited in the paper.
Y.-L. Wu, B. A. Bernevig, N. Regnault, Phys. Rev. B 85
2012
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S. Parameswaran, R. Roy, and S. Sondhi, Phys. Rev. B 85
2012
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T. Neupert, L. Santos, S. Ryu, C. Chamon, and C. Mudry, Phys. Rev. B 86
2012
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T. Neupert, L. Santos, C. Chamon, and C. Mudry, Phys. Rev. B 86
2012
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R. Roy, arXiv:1208.2055 (unpublished)
2055
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