Magnetotransport and thermoelectricity in disordered graphene
arXiv:cond-mat/0701714 · doi:10.1103/PhysRevB.76.035402
Abstract
We have studied the electric and thermal response of two-dimensional Dirac-fermions in a quantizing magnetic field in the presence of localized disorder. The electric and heat current operators in the presence of magnetic field are derived. The self-energy due to impurities is calculated self-consistently, and depends strongly on the frequency and field strength, resulting in asymmetric peaks in the density of states at the Landau level energies, and small islands connecting them. The Shubnikov-de Haas oscillations remain periodic in 1/B, in spite of the distinct quantization of quasiparticle orbits compared to normal metals. The Seebeck coefficient depends strongly on the field strength and orientation. For finite field and chemical potential, the Wiedemann-Franz law can be violated.
arXiv comment10 pages, 6 figures
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- Thermoelectric and Magnetothermoelectric Transport Measurements of Graphene
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- AC conductivity of graphene: from tight-binding model to 2+1-dimensional quantum electrodynamics
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- Impurity Scattering and Mott's Formula in Graphene
- Ultra-sensitive and Wide Bandwidth Thermal Measurements of Graphene at Low Temperatures
- Surface acoustic wave propagation in monolayer graphene
- Thermopower of gapped bilayer graphene
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- Thermoelectric effect in high mobility single layer epitaxial graphene
- Magnetotransport through graphene spin valves
- Thermoelectric and thermal transport in bilayer graphene systems
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- Thermopower of multilayer graphene
- High-energy Landau levels in graphene beyond nearest-neighbor hopping processes: Corrections to the effective Dirac Hamiltonian
- Stacking-order dependence in thermoelectric transport of biased trilayer graphene
- Quantum Corrections to Thermopower and Conductivity in Graphene
- Magnetothermoelectric transport in modulated and unmodulated graphene