Why the first magic-angle is different from others in twisted graphene bilayers: Interlayer currents, kinetic and confinement energy, and wave-function localization

The chiral Hamiltonian for twisted graphene bilayers is analyzed in terms of its squared Hamiltonian which removes the particle-hole symmetry and thus one bipartite lattice, allowing us to write the Hamiltonian in terms of a 2×2 matrix. This brings to the front the three main physical actors of twis...

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Bibliographic Details
Main Authors: Aguilar-Mendez, E. (Author), Espinosa-Champo, A. (Author), Naumis, G.G (Author), Navarro-Labastida, L.A (Author)
Format: Article
Language:English
Published: American Physical Society 2022
Subjects:
Online Access:View Fulltext in Publisher
LEADER 02503nam a2200349Ia 4500
001 10.1103-PhysRevB.105.115434
008 220425s2022 CNT 000 0 und d
020 |a 24699950 (ISSN) 
245 1 0 |a Why the first magic-angle is different from others in twisted graphene bilayers: Interlayer currents, kinetic and confinement energy, and wave-function localization 
260 0 |b American Physical Society  |c 2022 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1103/PhysRevB.105.115434 
520 3 |a The chiral Hamiltonian for twisted graphene bilayers is analyzed in terms of its squared Hamiltonian which removes the particle-hole symmetry and thus one bipartite lattice, allowing us to write the Hamiltonian in terms of a 2×2 matrix. This brings to the front the three main physical actors of twisted systems: kinetic energy, confinement potential, and an interlayer interaction operator which is divided in two parts: a non-Abelian interlayer operator and an operator which contains an interaction energy between layers. Here, each of these components is analyzed as a function of the angle of rotation as well as in terms of the wave-function localization properties. It is proved that the non-Abelian operator represents interlayer currents between each layer of triangular sublattices, i.e., a second-neighbor interlayer current between bipartite sublattices. A crossover is seen between such contributions, and thus, the first magic-angle is different from other higher-order magic-angles. Such angles are determined by a balance between the negative energy contribution from interlayer currents and the positive contributions from the kinetic and confinement energies. A perturbative analysis performed around the first magic-angle allows us to explore analytically the details of such an energy balance. © 2022 American Physical Society. 
650 0 4 |a Confinement energy 
650 0 4 |a 'current 
650 0 4 |a Current confinement 
650 0 4 |a Current energy 
650 0 4 |a Current kinetics 
650 0 4 |a Energy and wave functions 
650 0 4 |a Graphene 
650 0 4 |a Graphene bilayers 
650 0 4 |a Hamiltonians 
650 0 4 |a Kinetic energy 
650 0 4 |a Kinetics 
650 0 4 |a Localisation 
650 0 4 |a Magic angle 
650 0 4 |a Sub-lattices 
650 0 4 |a Wave functions 
700 1 |a Aguilar-Mendez, E.  |e author 
700 1 |a Espinosa-Champo, A.  |e author 
700 1 |a Naumis, G.G.  |e author 
700 1 |a Navarro-Labastida, L.A.  |e author 
773 |t Physical Review B