论文标题

与石墨烯相互作用的原子的Nernst HEAT定理:具有非零能隙和化学势的Dirac模型

The Nernst heat theorem for an atom interacting with graphene: Dirac model with nonzero energy gap and chemical potential

论文作者

Klimchitskaya, G. L., Mostepanenko, V. M.

论文摘要

对于具有非零的能量差距$δ$和化学势$μ$,我们得出了Casimir-Polder自由能的低温行为。石墨烯对电磁场的响应是通过dirac模型框架中的极化张量来描述了Matsubara公式中热量子场理论的第一原理。结果表明,对Casimir-Polder能量的热校正由三个贡献组成。其中的第一个由使用在零温度定义的极化张量的Matsubara求和确定,而第二和第三个贡献是由极化张量的明确温度依赖性引起的,并源自零频率Matsubara项以及所有MATSUBARA术语的总和,分别具有非零频率。在低温下,对于能量差距和化学势的任何值,在低温下的三个贡献中的每一个贡献的渐近行为都进行了分析。根据我们的结果,对于$δ>2μ$和$Δ<2μ$,满足了Casimir-Polder自由能和熵的Nernst Heat Heat定理。我们还揭示了在$δ=2μ$的情况下引起的熵异常。与Casimir物理学中有关物质对电磁场的介电响应的适当描述的长期基本问题的讨论讨论了所获得的结果。

We derive the low-temperature behavior of the Casimir-Polder free energy for a polarizable atom interacting with graphene sheet which possesses the nonzero energy gap $Δ$ and chemical potential $μ$. The response of graphene to the electromagnetic field is described by means of the polarization tensor in the framework of Dirac model on the basis of first principles of thermal quantum field theory in the Matsubara formulation. It is shown that the thermal correction to the Casimir-Polder energy consists of three contributions. The first of them is determined by the Matsubara summation using the polarization tensor defined at zero temperature, whereas the second and third contributions are caused by an explicit temperature dependence of the polarization tensor and originate from the zero-frequency Matsubara term and the sum of all Matsubara terms with nonzero frequencies, respectively. The asymptotic behavior for each of the three contributions at low temperature is found analytically for any value of the energy gap and chemical potential. According to our results, the Nernst heat theorem for the Casimir-Polder free energy and entropy is satisfied for both $Δ> 2μ$ and $Δ< 2μ$. We also reveal an entropic anomaly arising in the case $Δ= 2μ$. The obtained results are discussed in connection with the long-standing fundamental problem in Casimir physics regarding the proper description of the dielectric response of matter to the electromagnetic field.

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