Anisotropic Moiré Fractional Chern Insulators and Their Phase Transitions
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arXiv
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| Format: | Preprint |
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2026
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| _version_ | 1866914622890573824 |
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| author | Peng, Bo Hu, Jin-Xin |
| author_facet | Peng, Bo Hu, Jin-Xin |
| contents | Recently, moiré heterostructures have been observed to host fractional Chern insulator (FCI) phases at zero magnetic field. In this work, we show that the FCI phases are robust against moderate lattice anisotropy, while sufficiently strong anisotropy drives quantum phase transitions from incompressible topological phases to competing charge-density-wave (CDW) and Fermi-liquid (FL) phases. Specifically, in the case of twisted transition metal dichalcogenides (such as MoTe$_2$), the anisotropy arises from an interlayer momentum shift induced by heterostrain. We find that increasing anisotropy suppresses the many-body topological gap, eventually destabilizing the fractional topological phase. Beyond a critical anisotropy value, the system gradually transitions to a symmetry-broken state characterized by stripe-like CDW order. It has a Landau Level counterpart, where effective mass anisotropy provides an additional tuning knob for the fractional quantum Hall state; sufficiently strong anisotropy drives a transition to a charge-ordered phase. Moreover, in the anisotropic ideal Chern band model with lattice stretching, a Fermi liquid phase emerges as anisotropy increases. Our results establish that anisotropy provides a direct route for engineering and exploring competing correlated phases in FCI states based on moiré materials. |
| format | Preprint |
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arxiv_https___arxiv_org_abs_2606_02094 |
| institution | arXiv |
| publishDate | 2026 |
| record_format | arxiv |
| spellingShingle | Anisotropic Moiré Fractional Chern Insulators and Their Phase Transitions Peng, Bo Hu, Jin-Xin Strongly Correlated Electrons Recently, moiré heterostructures have been observed to host fractional Chern insulator (FCI) phases at zero magnetic field. In this work, we show that the FCI phases are robust against moderate lattice anisotropy, while sufficiently strong anisotropy drives quantum phase transitions from incompressible topological phases to competing charge-density-wave (CDW) and Fermi-liquid (FL) phases. Specifically, in the case of twisted transition metal dichalcogenides (such as MoTe$_2$), the anisotropy arises from an interlayer momentum shift induced by heterostrain. We find that increasing anisotropy suppresses the many-body topological gap, eventually destabilizing the fractional topological phase. Beyond a critical anisotropy value, the system gradually transitions to a symmetry-broken state characterized by stripe-like CDW order. It has a Landau Level counterpart, where effective mass anisotropy provides an additional tuning knob for the fractional quantum Hall state; sufficiently strong anisotropy drives a transition to a charge-ordered phase. Moreover, in the anisotropic ideal Chern band model with lattice stretching, a Fermi liquid phase emerges as anisotropy increases. Our results establish that anisotropy provides a direct route for engineering and exploring competing correlated phases in FCI states based on moiré materials. |
| title | Anisotropic Moiré Fractional Chern Insulators and Their Phase Transitions |
| topic | Strongly Correlated Electrons |
| url | https://arxiv.org/abs/2606.02094 |