2021
DOI: 10.1103/physrevresearch.3.013033
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Nematic topological semimetal and insulator in magic-angle bilayer graphene at charge neutrality

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Cited by 146 publications
(102 citation statements)
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“…These results are in agreement with another atomistic calculation which found that only retaining Hubbard interactions can only yield insulating states at charge neutrality [57,58], and also continuum model Hartree-Fock calculations that break C 2 symmetry [55]. To overcome the limitations of the current approach, future research should investigate longer-ranged exchange interactions [51][52][53][54][55][56] and the influence of ordering tendencies with q = 0 which could give rise to alternative symmetry-breaking mechanisms such as valley [9] and rotational [24] symmetry.…”
Section: Discussionsupporting
confidence: 86%
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“…These results are in agreement with another atomistic calculation which found that only retaining Hubbard interactions can only yield insulating states at charge neutrality [57,58], and also continuum model Hartree-Fock calculations that break C 2 symmetry [55]. To overcome the limitations of the current approach, future research should investigate longer-ranged exchange interactions [51][52][53][54][55][56] and the influence of ordering tendencies with q = 0 which could give rise to alternative symmetry-breaking mechanisms such as valley [9] and rotational [24] symmetry.…”
Section: Discussionsupporting
confidence: 86%
“…Experimentally, the situation is not clear, however, with some experiments reporting semimetallic behavior near the magic angle [1,2,4], while others (for very similar twist angles) observe a strong insulating state [5]. These conflicting results could arise from different levels of strain in the samples: Liu et al [53] demonstrated that a C 3 broken-symmetry state that is stabilized by strain retains its semimetallic character because of the topological properties of the flat bands of tBLG.…”
Section: Discussionmentioning
confidence: 99%
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“…The Hartree potential widens the bands, as it shifts the energies at the and points of the moiré Brillouin zone (BZ) with respect to those at the point ( 39 43 ). The inclusion of the exchange term in a full Hartree–Fock calculation leads to broken symmetry phases, with valley and/or spin polarization ( 44 47 ), among other possible phases (see also refs. 47 50 ).…”
Section: The Modelmentioning
confidence: 99%
“…The inclusion of the exchange term in a full Hartree–Fock calculation leads to broken symmetry phases, with valley and/or spin polarization ( 44 47 ), among other possible phases (see also refs. 47 50 ).…”
Section: The Modelmentioning
confidence: 99%