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A self-consistent Hartree theory for lattice-relaxed magic-angle twisted bilayer graphene
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abstract
For twisted bilayer graphene close to magic angle, we show that the effects of lattice relaxation and the Hartree interaction both become simultaneously important. Including both effects in a continuum theory reveals a Lifshitz transition to a Fermi surface topology that supports both a ``heavy fermion" pocket and an ultraflat band ($\approx 8~{\rm meV}$) that is pinned to the Fermi energy for a large range of fillings. We provide analytical and numerical results to understand the narrow ``magic angle range" that supports this pinned ultraflat band and make predictions for its experimental observation. We believe that the bands presented here are accurate at high temperature and provide a good starting point to understand the myriad of complex behaviour observed in this system.
Forward citations
Cited by 3 Pith papers
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The Interacting Energy Bands of Magic Angle Twisted Bilayer Graphene Revealed by the Quantum Twisting Microscope
A direct momentum-resolved image of the interacting bands of magic-angle twisted bilayer graphene reveals flat heavy-electron regions and dispersive light-electron regions that evolve with doping.
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Straintronics and twistronics in bilayer graphene
Strain shifts the angle of flattest bands, broadens flat bands roughly linearly, and can switch their valley topology from ±1 to 0, with shear strain acting more strongly than uniaxial.
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Many-body perturbation theory for moir\'{e} systems
A Green's function perturbation theory in the band basis gives analytical Hartree-Fock ground states for twisted bilayer graphene and shows self-consistent GW corrections reduce compressibility oscillations.
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