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Drude corrections to Casimir force calculations in liquids<br />

Raul Esquivel-Sirvent 1<br />

1 Instituto de Física, Universidad Nacioanl Autónoma de México, México D.F. 01000.<br />

Mo-1050<br />

The Casimir force for metals immersed in different fluids has been measured recently<br />

[1,2,3]. The comparison with theory is based on the Lifshitz formula and the knowledge<br />

<strong>of</strong> the dielectric function <strong>of</strong> the involved materials. In the case <strong>of</strong> the reported<br />

experiments, Au is a common metal used in the force measurements. The data for the<br />

dielectric function <strong>of</strong> Au can be obtained from tabulated data with a low frequency<br />

interpolation using the Drude model. The data for the optical properties <strong>of</strong> Au are usually<br />

measured in air or partial vacuum. However, changes in the Drude parameters <strong>of</strong> metals<br />

when immersed in fluids have been reported in the literature. Gugger [4] using the<br />

method <strong>of</strong> total attenuated internal reflection measured the dielectric function <strong>of</strong> Ag films<br />

in contact with different liquids. The measurements showed a change in the dielectric<br />

function <strong>of</strong> the Ag film depending on the index <strong>of</strong> refraction <strong>of</strong> the fluids. The same<br />

conclusion was reached in the work <strong>of</strong> Chen [5] that by means <strong>of</strong> spectroscopic<br />

ellipsometry measured the Drude parameters for Au and Ag films immersed in liquids,<br />

confirming the change in the Drude parameters <strong>of</strong> the metals.<br />

In this paper we examine the change in the Casimir force between two Au surfaces<br />

immersed in different fluids and how the change in the Drude parameters affects the<br />

Casimir force calculations. In particular, we show that variations <strong>of</strong> the order <strong>of</strong> 8% are<br />

possible and observed discrepancies between theory and experiment can be explained<br />

by this effect. The change <strong>of</strong> the Drude parameters <strong>of</strong> a metal immersed in a fluid are<br />

described by a Bruggeman effective medium theory. Finally, we discuss the possible<br />

applications <strong>of</strong> effective medium theories within the Lifshitz formalism.<br />

[1] J. N. Munday and F. Capasso, Phys. Rev. A 75, 060102(R) (2007).<br />

[2] J. N. Munday, F. Capasso, V. A. Parseguian and S. M. Bezrukov, Phys. Rev. A 78,<br />

029906 (2008).<br />

[3] P. J. van Zwol, G. Palasantzas and J. Th. M. De Hosson, Phys. Rev. B 79, 195428<br />

(2009).<br />

[4] H. Guger, M. Jurich and J. D. Swalen, Phys. Rev. B 30, 4189 (1984).<br />

[5] L. Y. Chen and D. W. Lynch, Phys. Rev. B 36, 1425 (1987).<br />

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