Correlations, Plasmarons, and Quantum Spectral Function in Bilayer Graphene
arXiv:1102.1427 · doi:10.1103/PhysRevB.84.041408
Abstract
We theoretically study the many-body effects of electron electron interaction on the single particle spectral function of doped bilayer graphene. Using random phase approximation, we calculate the real and imaginary part of the self-energy and hence the spectral function. The spectral function near the Fermi surface shows the usual quasiparticle peak, establishing doped bilayer graphene, in contrast to the unstable neutral system, to be a Fermi liquid. Away from the Fermi surface, an additional broad plasmaron peak is visible in the spectral function. From the low energy behaviour of the self-energy we calculate the quasiparticle residue and the effective mass of the quasiparticles as a function of carrier density. We present results for both the on-shell and the off-shell approximation for the quasiparticle renormalization.
5 pages, 3 figures
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- Effective Mass in Bilayer Graphene at Low Carrier Densities: the Role of Potential Disorder and Electron-Electron Interaction
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- Temperature-dependent compressibility in graphene and two-dimensional systems
- Effect of electron-phonon coupling on energy and density of states renormalizations of dynamically screened graphene
- Plasmon-pole approximation for many-body-effects in extrinsic graphene
- Excitonic gap formation and condensation in the bilayer graphene structure
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- Plasmons and their interaction with electrons in trilayer graphene
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- Distinguishing Coulomb and electron-phonon interactions for massless Dirac fermions
- Bilayer honeycomb lattice with ultracold atoms: Multiple Fermi surfaces and incommensurate spin density wave instability
- Electron-electron interactions in non-equilibrium bilayer graphene
- Many-body fermionic excitations in Weyl semimetals due to elastic gauge fields