Quantum field theoretical description of the Casimir effect between two
real graphene sheets and thermodynamics
- URL: http://arxiv.org/abs/2006.15557v2
- Date: Fri, 10 Jul 2020 15:16:38 GMT
- Title: Quantum field theoretical description of the Casimir effect between two
real graphene sheets and thermodynamics
- Authors: G. L. Klimchitskaya and V. M. Mostepanenko
- Abstract summary: Graphene is described in the framework of thermal quantum field theory in the Matsubara formulation.
Different expressions are found under the conditions $Delta>2mu$, $Delta=2mu$, and $Delta2mu$.
For both $Delta>2mu$ and $Delta2mu$ the Casimir entropy satisfies the third law of thermodynamics.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: The analytic asymptotic expressions for the Casimir free energy and entropy
for two parallel graphene sheets possessing nonzero energy gap $\Delta$ and
chemical potential $\mu$ are derived at arbitrarily low temperature. Graphene
is described in the framework of thermal quantum field theory in the Matsubara
formulation by means of the polarization tensor in (2+1)-dimensional
space-time. Different asymptotic expressions are found under the conditions
$\Delta>2\mu$, $\Delta=2\mu$, and $\Delta<2\mu$ taking into account both the
implicit temperature dependence due to a summation over the Matsubara
frequencies and the explicit one caused by a dependence of the polarization
tensor on temperature as a parameter. It is shown that for both $\Delta>2\mu$
and $\Delta<2\mu$ the Casimir entropy satisfies the third law of thermodynamics
(the Nernst heat theorem), whereas for $\Delta=2\mu$ this fundamental
requirement is violated. The physical meaning of the discovered anomaly is
considered in the context of thermodynamic properties of the Casimir effect
between metallic and dielectric bodies.
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