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One-loop omega-potential of quantum fields with ellipsoid constant-energy surface dispersion law

机译:具有椭球恒能表面色散定律的量子场的一环ω-势

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摘要

Rapidly convergent expansions of a one-loop contribution to the partition function of quantum fields with ellipsoid constant-energy surface dispersion law are derived. The omega-potential is naturally decomposed into three parts: the quasiclassical contribution, the contribution from the branch cut of the dispersion law, and the oscillating part. The low- and high-temperature expansions of the quasiclassical part are obtained. An explicit expression and a relation of the contribution from the cut with the Casimir term and vacuum energy are established. The oscillating part is represented in the form of the Chowla-Selberg expansion of the Epstein zeta function. Various resummations of this expansion are considered. The general procedure developed is then applied to two models: massless particles in a box both at zero and nonzero chemical potential, and electrons in a thin metal film. Rapidly convergent expansions of the partition function and average particle number are obtained for these models. In particular, the oscillations of the chemical potential of conduction electrons in graphene and a thin metal film due to a variation of size of the crystal are described.
机译:推导了单环对椭圆形恒能表面色散定律对量子场分配函数的快速收敛展开。 Ω势自然地分解为三个部分:准经典贡献,色散定律的分支切分的贡献和振荡部分。获得了准经典零件的低温和高温膨胀。建立了明确的表达式,以及切口的贡献与卡西米尔项和真空能之间的关系。振荡部分以爱泼斯坦zeta函数的Chowla-Selberg展开形式表示。考虑了这种扩展的各种恢复。然后将开发的一般程序应用于两个模型:处于零化学势和非零化学势的盒子中的无质量粒子,以及金属薄膜中的电子。对于这些模型,获得了分配函数和平均粒子数的快速收敛展开。特别地,描述了由于晶体尺寸的变化而导致的石墨烯和金属薄膜中的传导电子的化学势的振荡。

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