Casimir interaction of strained graphene
arXiv:1703.02500 · doi:10.1016/j.physleta.2017.05.040
Abstract
We calculate the Casimir interaction of two freestanding graphene samples under uniaxial strain. Our approach fully takes retardation and dispersion into account and is based on quantum field theoretical expressions for conductivities in terms of the polarization operator. The force shows a rather weak dependence on the realistic values of strain, changing just by a few percent in its maximum as compared to the non-strained case.
5 pages, 3 figures, EPL style, misprint corrected
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Cited by in corpus (7)
- The quest for Casimir repulsion between Chern-Simons surfaces
- Casimir and Casimir-Polder Forces in Graphene Systems: Quantum Field Theoretical Description and Thermodynamics
- The Casimir effect for fermionic currents in conical rings with applications to graphene ribbons
- The Casimir effect in graphene systems: Experiment and theory
- On the convergence of the polarization tensor in space-time of three dimensions
- Casimir effect for fermion condensate in conical rings
- Temperature Dependence of the Response Functions of Graphene: Impact on Casimir and Casimi-Polder Forces in and out of Thermal Equilibrium