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Classical Casimir-Polder force between polarizable microparticles and thin films including graphene

机译:极化微粒与极化之间的古典Casimir-polder力   薄膜包括石墨烯

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摘要

We derive analytic expressions for the classical Casimir-Polder free energyand force for a polarizable (magnetizable) atom (microparticle) interactingwith thin films, made of different materials, or graphene. It is shown that foran isolated dielectric film the free energy and force decrease quicker withseparation, as compared to the case of atom interacting with a thick plate(semispace). For metallic films some peculiar features depending on the modelof a metal used are analyzed. For an atom interacting with graphene wedemonstrate that at room temperature the classical regime is achieved at about$1.5\,\mu$m separation. In this regime the contributions to the free energy andforce due to atomic magnetic polarizability are suppressed, as compared to mainterms caused by the atomic electric polarizability. According to our results,at separations above $5\,\mu$m the Casimir-Polder interaction of atoms withgraphene is of the same strength as with an ideal-metal plane. The classicalinteraction of atoms with thin films deposited on substrates is alsoconsidered.
机译:我们推导了经典Casimir-Polder自由能和与不同材料或石墨烯制成的薄膜相互作用的可极化(可磁化)原子(微粒)的力的解析表达式。结果表明,与原子与厚板(半空间)相互作用的情况相比,对于隔离的介电膜,自由能和作用力随着分离而更快地降低。对于金属膜,根据所用金属的型号,分析了一些特殊的特征。对于与石墨烯相互作用的原子,我们可以证明在室温下经典的分离机理约为1.5μm。在这种情况下,与原子电极化率引起的主要项相比,由于原子磁极化率对自由能和力的贡献得到了抑制。根据我们的结果,当间距大于5μm时,原子与石墨烯的Casimir-Polder相互作用具有与理想金属平面相同的强度。还考虑了原子与沉积在基板上的薄膜的经典相互作用。

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