Van der Waals and Casimir interactions between two graphene sheets
arXiv:1302.5107 · doi:10.1103/PhysRevB.87.075439
Abstract
The thermal free energy and pressure of dispersion interaction between two graphene sheets described by the Dirac model are calculated using the Lifshitz formula with reflection coefficients expressed via the polarization tensor. The obtained results for a pristine graphene are found to be in agreement with computations using Coulomb coupling between density fluctuations. For a graphene with nonzero mass gap parameter a qualitatively different behavior for the free energy and pressure is obtained. The Lifshitz formula with reflection coefficients expressed via the polarization tensor is used as a test for different computational approaches proposed in the literature for modeling the response function and conductivity of graphene at both zero and nonzero temperature.
14 pages, 5 figures, to appear in Phys. Rev. B
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- Thermal effect in the Casimir force for graphene and graphene-coated substrates: Impact of nonzero mass gap and chemical potential
- Numerical calculation of the Casimir-Polder interaction between a graphene sheet with vacancies and an atom
- Comparison of hydrodynamic model of graphene with recent experiment on measuring the Casimir interaction
- Quantum electrodynamic approach to the conductivity of gapped graphene
- Casimir effects in systems containing 2D layers, like graphene and 2D electron gases
- Nernst heat theorem for the thermal Casimir interaction between two graphene sheets
- Casimir energy for surfaces with constant conductivity
- Optical properties of dielectric plates coated with gapped graphene
- Novel approaches to tailor and tune light-matter interactions at the nanoscale