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Finite temperature Casimir energy in closed rectangular cavities: a rigorous derivation based on a zeta function technique

机译:封闭矩形腔中的有限温度卡西米尔能量:基于zeta函数技术的严格推导

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We derive rigorously explicit formulae of the Casimir free energy at finite temperature for massless scalar field and electromagnetic field confined in a closed rectangular cavity with different boundary conditions by a zeta regularization method. We study both the low and high temperature expansions of the free energy. In each case, we write the free energy as a sum of a polynomial in temperature plus exponentially decay terms. We show that the free energy is always a decreasing function of temperature. In the cases of massless scalar field with the Dirichlet boundary condition and electromagnetic field, the zero temperature Casimir free energy might be positive. In each of these cases, there is a unique transition temperature (as a function of the side lengths of the cavity) where the Casimir energy changes from positive to negative. When the space dimension is equal to two and three, we show graphically the dependence of this transition temperature on the side lengths of the cavity. Finally we also show that we can obtain the results for a non-closed rectangular cavity by letting the size of some directions of a closed cavity go to infinity, and we find that these results agree with the usual integration prescription adopted by other authors.
机译:我们通过zeta正则化方法,严格限制了在有限边界条件下封闭的矩形腔中无质量的标量场和电磁场的卡西米尔自由能的精确公式。我们研究自由能的低温和高温膨胀。在每种情况下,我们将自由能写为温度多项式加指数衰减项的总和。我们表明,自由能始终是温度的下降函数。在具有Dirichlet边界条件和电磁场的无质量标量场的情况下,零温度卡西米尔自由能可能为正。在每种情况下,都有一个独特的转变温度(取决于腔体的边长),卡西米尔能量从正变到负。当空间尺寸等于2和3时,我们以图形方式显示了此转变温度对型腔侧面长度的依赖性。最后,我们还表明,通过使闭合空腔的某些方向的大小达到无穷大,可以获得非闭合矩形空腔的结果,并且我们发现这些结果与其他作者采用的通常的积分公式一致。

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