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Casimir and casimir-polder forces in graphene systems: Quantum field theoretical description and thermodynamics

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dc.contributor.author Klimchitskaya G.L.
dc.contributor.author Mostepanenko V.M.
dc.date.accessioned 2021-02-25T06:44:14Z
dc.date.available 2021-02-25T06:44:14Z
dc.date.issued 2020
dc.identifier.uri https://dspace.kpfu.ru/xmlui/handle/net/161015
dc.description.abstract © 2020 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/). We review recent results on the low-temperature behaviors of the Casimir-Polder and Casimir free energy an entropy for a polarizable atom interacting with a graphene sheet and for two graphene sheets, respectively. These results are discussed in the wide context of problems arising in the Lifshitz theory of van der Waals and Casimir forces when it is applied to metallic and dielectric bodies. After a brief treatment of different approaches to theoretical description of the electromagnetic response of graphene, we concentrate on the derivation of response function in the framework of thermal quantum field theory in the Matsubara formulation using the polarization tensor in (2 + 1)-dimensional space—time. The asymptotic expressions for the Casimir-Polder and Casimir free energy and entropy at low temperature, obtained with the polarization tensor, are presented for a pristine graphene as well as for graphene sheets possessing some nonzero energy gap ∆ and chemical potential µ under different relationships between the values of ∆ and µ. Along with reviewing the results obtained in the literature, we present some new findings concerning the case µ 6= 0, ∆ = 0. The conclusion is made that the Lifshitz theory of the Casimir and Casimir-Polder forces in graphene systems using the quantum field theoretical description of a pristine graphene, as well as real graphene sheets with ∆ > 2µ or ∆ < 2µ, is consistent with the requirements of thermodynamics. The case of graphene with ∆ = 2µ 6= 0 leads to an entropic anomaly, but is argued to be physically unrealistic. The way to a resolution of thermodynamic problems in the Lifshitz theory based on the results obtained for graphene is discussed.
dc.subject Casimir free energy
dc.subject Casimir-Polder free energy
dc.subject Entropy
dc.subject Nernst heat theorem
dc.subject Polarization tensor
dc.subject Quantum field theory
dc.subject Thermal correction
dc.title Casimir and casimir-polder forces in graphene systems: Quantum field theoretical description and thermodynamics
dc.type Review
dc.relation.ispartofseries-issue 9
dc.relation.ispartofseries-volume 6
dc.collection Публикации сотрудников КФУ
dc.source.id SCOPUS-2020-6-9-SID85091935487


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  • Публикации сотрудников КФУ Scopus [24551]
    Коллекция содержит публикации сотрудников Казанского федерального (до 2010 года Казанского государственного) университета, проиндексированные в БД Scopus, начиная с 1970г.

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