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

机译:可极化微粒与包括石墨烯的薄膜之间的经典Casimir-Polder力

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摘要

We derive analytic expressions for the classical Casimir-Polder free energy and force for a polarizable (magnetizable) atom (microparticle) interacting with thin films, made of different materials, or graphene. It is shown that for an isolated dielectric film the free energy and force decrease quicker with separation compared to the case of an atom interacting with a thick plate (semispace). For metallic films some peculiar features depending on the model of the metal used are analyzed. For an atom interacting with graphene we demonstrate that at room temperature the classical regime is achieved at about 1.5-μm separation. In this regime the contributions to the free energy and force due to atomic magnetic polarizability are suppressed compared to the main terms caused by the atomic electric polarizability. According to our results, at separations above 5μm the Casimir-Polder interaction of atoms with graphene is of the same strength as with an ideal-metal plane. The classical interaction of atoms with thin films deposited on substrates is also considered.
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,我们证明了在室温下,经典机理是在约1.5μm的分离下实现的。在这种情况下,与由原子电极化率引起的主要项相比,抑制了由于原子磁极化率对自由能和力的贡献。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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