2022
DOI: 10.48550/arxiv.2203.09188
|View full text |Cite
Preprint
|
Sign up to set email alerts
|

Electronic properties of twisted multilayer graphene

V. Hung Nguyen,
Trinh X. Hoang,
J. -C. Charlier

Abstract: Twisted bilayer graphene displays many fascinating properties that can be tuned by varying the relative angle (also called twist angle) between its monolayers. As a remarkable feature, both the electronic flat bands and the corresponding strong electron localization have been obtained at a specific "magic" angle (∼ 1.1 • ), leading to the observation of several strongly correlated electronic phenomena. Such a discovery has hence inspired the creation of a novel research field called twistronics, i.e., aiming t… Show more

Help me understand this report
View published versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

0
3
0

Year Published

2022
2022
2022
2022

Publication Types

Select...
1
1

Relationship

0
2

Authors

Journals

citations
Cited by 2 publications
(3 citation statements)
references
References 62 publications
(110 reference statements)
0
3
0
Order By: Relevance
“…starting from the Wannier representation Blochband Hamiltonian H XX ′ (K : d(r i )) = j t inter ij e iK•r ij [16,17] where X ( ′) is A or B sublattice of bottom(top) layer and the interlayer hopping parameter t inter ij is defined in equation (9). The integration runs over a moire commensurate cell of area A M , and we include both in-plane(u) and out-of-plane(h) stacking deformation d(r) = d 0 (r) + u(r) + h(r)ẑ where d 0 (r) is the rigid relative stacking information [18].…”
Section: Continuum Model Calculationsmentioning
confidence: 99%
See 1 more Smart Citation
“…starting from the Wannier representation Blochband Hamiltonian H XX ′ (K : d(r i )) = j t inter ij e iK•r ij [16,17] where X ( ′) is A or B sublattice of bottom(top) layer and the interlayer hopping parameter t inter ij is defined in equation (9). The integration runs over a moire commensurate cell of area A M , and we include both in-plane(u) and out-of-plane(h) stacking deformation d(r) = d 0 (r) + u(r) + h(r)ẑ where d 0 (r) is the rigid relative stacking information [18].…”
Section: Continuum Model Calculationsmentioning
confidence: 99%
“…Twisted graphene systems have emerged as the prime target and candidate for finding correlated electronic phenomena in 2D materials including flat band superconductivity [1][2][3][4][5][6]. Research has expanded beyond the initial investigation of twisted bilayer graphene (t2G) [1] to include a variety of other layered moire materials that have shown hints of similar physics [7][8][9]. Alternating twist N-layer graphene (tNG) systems are particularly interesting for exploring correlation physics in light of recent experiments that have revealed flat band superconductivity for N = 3, 4, 5 systems [3,10,11].…”
Section: Introductionmentioning
confidence: 99%
“…Twisted graphene systems have emerged as the prime target and candidate for finding correlated electronic phenomena in 2D materials including flat band superconductivity [1,2,3,4,5,6]. Research has expanded beyond the initial investigation of twisted bilayer graphene (t2G) [1] to include a variety of other layered moire materials that have shown hints of similar physics [7,8,9]. Alternating twist 𝑁layer graphene (t𝑁G) systems are particularly interesting for exploring correlation physics in light of recent experiments that have revealed flat band superconductivity for 𝑁 = 3, 4, 5 systems [10,3,11].…”
Section: Introductionmentioning
confidence: 99%