Fractional Chern insulator

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Fractional Chern insulators (FCIs) are lattice generalizations of the fractional quantum Hall effect that have been studied theoretically since 1993 [1] and have been studied more intensely since early 2010. [2] [3] They were first predicted to exist in topological flat bands carrying Chern numbers. They can appear in topologically non-trivial band structures even in the absence of the large magnetic fields needed for the fractional quantum Hall effect. In principle, they can also occur in partially filled bands with trivial band structures if the inter-electron interaction is unusual. [4] They promise physical realizations at lower magnetic fields, higher temperatures, and with shorter characteristic length scales compared to their continuum counterparts. [5] [6] FCIs were initially studied by adding electron-electron interactions [7] to a fractionally filled Chern insulator, in one-body models where the Chern band is quasi-flat, [8] [9] at zero magnetic field. The FCIs exhibit a fractional quantized Hall conductance.

Contents

Prior work and experiments with finite magnetic fields

In works predating the theoretical studies of FCIs, the analogue of the Laughlin state was demonstrated in Hofstadter-type models. [10] [11] The essential features of the topology of single-particle states in such models still stems from the presence of a magnetic field. Nevertheless, it was shown that in the presence of a lattice, fractional quantum Hall states can retain their topological character, in the form of fractional Chern numbers [12] . Chern Insulators - single-particle states exhibiting an integer anomalous quantized Hall effect at zero field - have been theoretically proposed. [13] Fractionally filling such states, in the presence of repulsive interactions, can lead to the zero-field Fractional Chern Insulator. These FCIs are sometimes not connected to the Fractional Quantum Hall Effect in Landau Levels. This is the case in bands with Chern number , [14] and are therefore a new type of states inherent to such lattice models. They have been explored with respect to their quasi-charge excitations, non-Abelian states and the physics of twist defects, [15] which may be conceptually interesting for topological quantum computing.

Experimentally, Chern insulators have been realized without a magnetic field. [16] FCIs have been claimed to be realized experimentally in van der Waals heterostructures, but with an external magnetic field of order 10 – 30 T and, more recently, FCIs in a band have been claimed to be observed in twisted bilayer graphene close to the magic angle, yet again requiring a magnetic field, of order 5 T in order to "smoothen" out the Berry curvature of the bands. [17] These states have been called FCIs due to their link to lattice physics -- either in Hofstadter bands or in the moiré structure, but still required nonzero-magnetic field for their stabilization.

Zero field fractional Chern insulators

The prerequisite of zero field fractional Chern insulator is magnetism. The best way to have magnetism is to have exchange interaction that simultaneously polarize the spin. This phenomenon in twisted MoTe2 in both integer and fractional states was first observed by a University of Washington group. [18] In 2023 a series of groups have reported FCIs at zero magnetic field [19] in twisted MoTe
2 samples. The University of Washington group [20] first identified fractional Chern number of , and state with trion emission sensing. This is followed by the Cornell group who performed thermodynamic measurement on and state. These samples, where the moiré bands are valley-spin locked, undergo a spin-polarization transition which gives rise to a Chern insulator state at integer filling of the moiré bands. Upon fractional filling at and , a gapped state develops with a fractional slope in the Streda formula, a hallmark of an FCI. These fractional states are identical to the predicted zero magnetic field FCIs. [7] After the optical sensing measurement, University of Washington group [21] first reported transport `smoking-gun` evidence of fractional quantum anomalous Hall effect that should be exhibited by a zero-field fractional Chern insulator at , and . They also identified a possible composite Fermi liquid at that mimics the half filled Landau level for 2D electron gas. The and states are also partially repeated by the Shanghai group, while the quantization is not as good. [22] The full matching of FCI physics in MoTe
2, using the single particle model proposed in, [23] to experiments still holds intriguing and unresolved mysteries. These were only partially theoretically addressed, [24] where the issues of model parameters, sample magnetization, and the appearance of some FCI states (at filling and ) but the absence of others (so far at filling at ) are partially addressed.

In graphene system, MIT group found the unexpected FCIs with lots of fractions in rhombohedral pentalayer graphene (RPG), which marks RPG another promising system for FCI physics with higher mobility and device quality.

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References

  1. ↑ Kol, A.; Read, N. (Sep 1993). "Fractional quantum Hall effect in a periodic potential". Physical Review B. 48 (12): 8890. doi:10.1103/PhysRevB.48.8890.
  2. ↑ Neupert, Titus; Chamon, Claudio; Iadecola, Thomas; Santos, Luiz H; Mudry, Christopher (2015-12-01). "Fractional (Chern and topological) insulators". Physica Scripta. T164: 014005. arXiv: 1410.5828 . Bibcode:2015PhST..164a4005N. doi:10.1088/0031-8949/2015/T164/014005. ISSN   0031-8949. S2CID   117125248.
  3. ↑ Liu, Zhao; Bergholtz, Emil J. (2024-01-01), "Recent developments in fractional Chern insulators", in Chakraborty, Tapash (ed.), Encyclopedia of Condensed Matter Physics (Second Edition), Oxford: Academic Press, pp. 515–538, arXiv: 2208.08449 , doi:10.1016/b978-0-323-90800-9.00136-0, ISBN   978-0-323-91408-6, S2CID   251643711 , retrieved 2023-11-05
  4. ↑ Simon, Steven H.; Harper, Fenner; Read, N. (2015-11-03). "Fractional Chern insulators in bands with zero Berry curvature". Physical Review B. 92: 195104.
  5. ↑ Bergholtz, Emil J.; Liu, Zhao (2013-09-30). "Topological Flat Band Models and Fractional Chern Insulators". International Journal of Modern Physics B. 27 (24): 1330017. arXiv: 1308.0343 . Bibcode:2013IJMPB..2730017B. doi:10.1142/S021797921330017X. ISSN   0217-9792. S2CID   119282096.
  6. ↑ Parameswaran, Siddharth A.; Roy, Rahul; Sondhi, Shivaji L. (2013-11-01). "Fractional quantum Hall physics in topological flat bands". Comptes Rendus Physique. Topological insulators / Isolants topologiques. 14 (9): 816–839. arXiv: 1302.6606 . Bibcode:2013CRPhy..14..816P. doi:10.1016/j.crhy.2013.04.003. ISSN   1631-0705. S2CID   117851815.
  7. 1 2 T. Neupert, L. Santos, C. Chamon, and C. Mudry, Phys. Rev. Lett. 106, 236804 (2011); D. N. Sheng, Z.-C. Gu, K. Sun, and L. Sheng, Nature Communications 2, 389 (2011); N. Regnault and B. A. Bernevig, Phys. Rev. X 1, 021014 (2011)
  8. ↑ Tang, Evelyn; Mei, Jia-Wei; Wen, Xiao-Gang (6 June 2011). "High-Temperature Fractional Quantum Hall States". Physical Review Letters. 106 (23): 236802. arXiv: 1012.2930 . Bibcode:2011PhRvL.106w6802T. doi: 10.1103/PhysRevLett.106.236802 . eISSN   1079-7114. ISSN   0031-9007. PMID   21770532.
  9. ↑ Sun, Kai; Gu, Zhengcheng; Katsura, Hosho; Das Sarma, S. (6 June 2011). "Nearly Flatbands with Nontrivial Topology". Physical Review Letters. 106 (23): 236803. arXiv: 1012.5864 . Bibcode:2011PhRvL.106w6803S. doi: 10.1103/PhysRevLett.106.236803 . eISSN   1079-7114. ISSN   0031-9007. PMID   21770533.
  10. ↑ Hafezi, M.; Sørensen, A. S.; Demler, E.; Lukin, M. D. (28 August 2007). "Fractional quantum Hall effect in optical lattices". Physical Review A. 76 (2): 023613. arXiv: 0706.0757 . Bibcode:2007PhRvA..76b3613H. doi:10.1103/PhysRevA.76.023613. eISSN   1094-1622. ISSN   1050-2947.
  11. ↑ Möller, G.; Cooper, N. R. (4 September 2009). "Composite Fermion Theory for Bosonic Quantum Hall States on Lattices". Physical Review Letters. 103 (10): 105303. arXiv: 0904.3097 . Bibcode:2009PhRvL.103j5303M. doi:10.1103/PhysRevLett.103.105303. eISSN   1079-7114. ISSN   0031-9007. PMID   19792327.
  12. ↑ Hafezi, M.; Sørensen, A. S.; Lukin, M. D.; Demler, E. (27 November 2007). "Characterization of topological states on a lattice with Chern number". Europhysics Letters (EPL). 81 (1): 10005. doi:10.1209/0295-5075/81/10005.
  13. ↑ Haldane, F. D. M. (31 October 1988). "Model for a Quantum Hall Effect without Landau Levels: Condensed-Matter Realization of the "Parity Anomaly"". Physical Review Letters. 61 (18): 2015–2018. doi: 10.1103/PhysRevLett.61.2015 . ISSN   0031-9007. PMID   10038961.
  14. ↑ Z. Liu, E. J. Bergholtz, H. Fan, and A. M. La ̈uchli, Phys. Rev. Lett. 109, 186805 (2012); A. Sterdyniak, C. Repellin, B. A. Bernevig, and N. Regnault Phys. Rev. B 87, 205137 (2013). M. Udagawa and E. J. Bergholtz, Journal of Statistical Mechanics: Theory and Experiment 2014, P10012 (2014); Y.-H. Wu, J. K. Jain, and K. Sun, Phys. Rev. B 91, 041119 (2015); G. Mo ̈ller and N. R. Cooper, Phys. Rev. Lett. 115, 126401(2015); B. Andrews and G. Mo ̈ller, Phys. Rev. B 97, 035159 (2018).
  15. ↑ B. d. z. Jaworowski, N. Regnault, and Z. Liu, Phys. Rev. B 99, 045136 (2019); M. Barkeshli and X.-L. Qi, Phys. Rev. X 2, 031013 (2012); E. J. Bergholtz, Z. Liu, M. Trescher, R. Moessner, and M. Udagawa, Phys. Rev. Lett. 114, 016806 (2015); Z. Liu, G. Möller, and E. J. Bergholtz, Phys. Rev. Lett. 119, 106801 (2017).
  16. ↑ G. Chen, A. L. Sharpe, E. J. Fox, Y.-H. Zhang, S. Wang, L. Jiang, B. Lyu, H. Li, K. Watanabe, T. Taniguchi, Z. Shi,T. Senthil, D. Goldhaber-Gordon, Y. Zhang, and F. Wang, Nature 579, 56 (2020)
  17. ↑ E. M. Spanton, A. A. Zibrov, H. Zhou, T. Taniguchi, K. Watanabe, M. P. Zaletel, and A. F. Young, Science 360, 62 (2018), https://science.sciencemag.org/content/360/6384/62.full.pdf; Y. Xie, A. T. Pierce, J. M. Park, D. E. Parker, E. Khalaf, P. Ledwith, Y. Cao, S. H. Lee, S. Chen, P. R. Forrester, K. Watanabe, T. Taniguchi, A. Vishwanath, P. Jarillo- Herrero, and A. Yacoby, Nature 600, 439 (2021).
  18. ↑ Anderson, Eric, Feng-Ren Fan, Jiaqi Cai, William Holtzmann, Takashi Taniguchi, Kenji Watanabe, Di Xiao, Wang Yao, and Xiaodong Xu. "Programming correlated magnetic states with gate-controlled moiré geometry." Science (2023): eadg4268.
  19. ↑ J. Cai, E. Anderson, C. Wang, X. Zhang, X. Liu, W. Holtzmann, Y. Zhang, F. Fan, T. Taniguchi, K. Watanabe, Y. Ran, T. Cao, L. Fu, D. Xiao, W. Yao, and X. Xu, Nature (2023), Nature volume 622, pages 63-68; Y. Zeng, Z. Xia, K. Kang, J. Zhu, P. Knu ̈ppel, C. Vaswani, K. Watanabe, T. Taniguchi, K. F. Mak, and J. Shan, “Thermodynamic evidence of fractional Chern insulator in moiré MoTe
    2    ,” (2023), Nature volume 622, pages 69–73 (2023); Heonjoon Park, Jiaqi Cai, Eric Anderson, Yinong Zhang, Jiayi Zhu, Xiaoyu Liu, Chong Wang et al. "Observation of fractionally quantized anomalous Hall effect." Nature 622, no. 7981 (2023): 74-79.
  20. ↑ J. Cai, E. Anderson, C. Wang, X. Zhang, X. Liu, W. Holtzmann, Y. Zhang, F. Fan, T. Taniguchi, K. Watanabe, Y. Ran, T. Cao, L. Fu, D. Xiao, W. Yao, and X. Xu, Nature (2023), Nature volume 622, pages 63-68
  21. ↑ Heonjoon Park, Jiaqi Cai, Eric Anderson, Yinong Zhang, Jiayi Zhu, Xiaoyu Liu, Chong Wang et al. "Observation of fractionally quantized anomalous Hall effect." Nature 622, no. 7981 (2023): 74-79.
  22. ↑ Xu, Fan, et al. "Observation of integer and fractional quantum anomalous Hall effects in twisted bilayer MoTe 2." Physical Review X 13.3 (2023): 031037.
  23. ↑ F. Wu, T. Lovorn, E. Tutuc, I. Martin, and A. H. Mac- Donald, Phys. Rev. Lett. 122, 086402 (2019)
  24. ↑ C. Wang, X.-W. Zhang, X. Liu, Y. He, X. Xu, Y. Ran, T. Cao, and D. Xiao, “Fractional chern insulator in twisted bilayer MoTe
    2    ,” (2023), arXiv:2304.11864 [cond-mat.str-el]; V. Cr ́epel and L. Fu, "Anomalous Hall metal and fractional Chern insulator in twisted transition metal dichalcogenides," Phys. Rev. B 107, L201109 (2023); N. Morales-Dura ́n, J. Wang, G. R. Schleder, M. Angeli, Z. Zhu, E. Kaxiras, C. Repellin, and J. Cano, “Pressure–enhanced fractional chern insulators in moiré transition metal dichalcogenides along a magic line,” (2023), arXiv:2304.06669 [cond-mat.str-el]; N. Morales-Dura ́n, N. Wei, and A. H. MacDonald, “Magic angles and fractional chern insulators in twisted homobilayer tmds,” (2023), arXiv:2308.03143 [cond-mat.str-el]; J. Yu, J. Herzog-Arbeitman, M. Wang, O. Vafek, B. A. Bernevig, and N. Regnault, “Fractional chern insulators vs. non-magnetic states in twisted bilayer MoTe
    2    ,” (2023), arXiv:2309.14429 [cond-mat.mes-hall]
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