Energy gaps at neutrality point in bilayer graphene in a magnetic field
arXiv:0910.5459 · doi:10.1134/S0021364010060111
Abstract
Utilizing the Baym-Kadanoff formalism with the polarization function calculated in the random phase approximation, the dynamics of the quantum Hall state in bilayer graphene is analyzed. Two phases with nonzero energy gap, the ferromagnetic and layer asymmetric ones, are found. The phase diagram in the plane , where is a top-bottom gates voltage imbalance, is described. It is shown that the energy gap scales linearly, $ΔE\sim 14 B[T]K, with magnetic field.
5 pages, 3 figures, title changed, references added, JETP Letters version
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Cited by in corpus (23)
- Quantum field theory in a magnetic field: From quantum chromodynamics to graphene and Dirac semimetals
- Spontaneously gapped ground state in suspended bilayer graphene
- Local Compressibility Measurements of Correlated States in Suspended Bilayer Graphene
- Magnetic Catalysis: A Review
- Topological Phases in the Zeroth Landau Level of Bilayer Graphene
- Dynamical screening in bilayer graphene
- New Dirac points and multiple Landau level crossings in biased trilayer graphene
- Broken-symmetry quantum Hall states in bilayer graphene: Landau level mixing and dynamical screening
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- Broken-symmetry states and phase diagram of the lowest Landau level in bilayer graphene
- Renormalization group aspects of graphene
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- Spin-orbit proximity in MoS/bilayer graphene heterostructures
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- Effect of the band structure topology on the minimal conductivity for bilayer graphene with symmetry breaking
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- Gap generation in ABC-stacked multilayer graphene: screening vs band flattening
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- Phase diagram of a graphene bilayer in the zero-energy Landau level
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- Ising quantum Hall ferromagnetism in Landau levels of bilayer graphene
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