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An unconventional insulating phase and a superconducting phase were recently discovered in the twisted bilayer graphene [Y.
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K. Kim, A. DaSilva, S. Huang, B. Fallahazad, S. Larentis, T. Taniguchi, K. Watanabe, B. J. LeRoy, A. H. MacDonald, and E. Tutuc, “Tunable moiré bands and strong correlations in small-twist-angle bilayer graphene,” Proc. Natl. Acad. Sci. 114
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A. Ramires and J. L. Lado, “Electrically tunable gauge fields in tiny-angle twisted bilayer graphene,” Phys. Rev. Lett. 121
2018
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C. Xu and L. Balents, “Topological Superconductivity in Twisted Multilayer Graphene,” Phys. Rev. Lett. 121
2018
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Y. Cao, V. Fatemi, A. Demir, S. Fang, S. L. Tomarken, J. Y. Luo, J. D. Sanchez-Yamagishi, K. Watanabe, T. Taniguchi, E. Kaxiras, R. C. Ashoori, and P. Jarillo-Herrero, “Correlated insulator behaviour at half-filling in magic-angle graphene superlattices,” Nature 556
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Y. Cao, V. Fatemi, S. Fang, K. Watanabe, T. Taniguchi, E. Kaxiras, and P. Jarillo-Herrero, “Unconventional superconductivity in magic-angle graphene superlattices,” Nature 556
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The renormalized Dirac velocity is denoted by \mathaccentV t i l d e 07 E v F \mathaccentV{tilde}07E{v}_{F} instead of v F ∗ v_{F}^{*} in Ref. [ 14 ] . The superscript ∗
Cited in the paper.
The precise asymptotic form of f ( r ) f(r) is not significant because, as shown in the main text, the zero mode wavefunction at long distance is exponentially suppressed as \mathaccentV t i l d e 07 E v F \mathaccentV{tilde}07E{v}_{F} vanishes at the magic angles
Cited in the paper.
2018
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D. K. Efimkin and A. H. MacDonald, “Helical network model for twisted bilayer graphene,” Phys. Rev. B 98
2018
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J. González and T. Stauber, “Kohn-Luttinger superconductivity in twisted bilayer graphene,” Phys. Rev. Lett. 122
2019
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