Possibility to measure thermal effects in the Casimir force

Abstract

We analyze the possibility to measure small thermal effects in the Casimir force between metal test bodies in configurations of a sphere above a plate and two parallel plates. For sphere-plate geometry used in many experiments we investigate the applicability of the proximity force approximation (PFA) to calculate thermal effects in the Casimir force and its gradient. It is shown that for real metals the two formulations of the PFA used in the literature lead to relative differences in the obtained results being less than a small parameter equal to the ratio of separation distance to sphere radius. For ideal metals the PFA results for the thermal correction are obtained and compared with available exact results. It is emphasized that in the experimental region in the zeroth order of the small parameter mentioned above the thermal Casimir force and its gradient calculated using the PFA (and thermal corrections in their own right) coincide with respective exact results. For real metals available exact results are outside the application region of the PFA. However, the exact results are shown to converge to the PFA results when the small parameter goes down to the experimental values. We arrive at the conclusion that large thermal effects predicted by the Drude model approach, if existing at all, could be measured in both static and dynamic experiments in sphere-plate and plate-plate configurations. As to the small thermal effects predicted by the plasma model approach, the static experiment in the configuration of two parallel plates is found to be the best for its observation.

35 pages, 9 figures; Phys. Rev. A, to appear

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Cited by in corpus (5)

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• Control of the Casimir Force Using Semiconductor Test Bodies
• Exact Casimir-Polder potential between a particle and an ideal metal cylindrical shell and the proximity force approximation
• Casimir interaction of concentric spheres at finite temperature
• Some Developments of the Casimir Effect in $p$-Cavity of $(D+1)$-Dimensional Spacetime