Abstract:We derive an exact analytic expression for the high-temperature limit of the
Casimir interaction between two Drude spheres of arbitrary radii. Specifically,
we determine the Casimir free energy by using the scattering approach in the
plane-wave basis. Within a round-trip expansion, we are led to consider the
combinatorics of certain partitions of the round trips. The
relation between the Casimir free energy and the capacitance matrix of two
spheres is discussed. Previously known results for the special cases … Show more
“…At vanishing frequency, the reflection matrix elements of the sphere are diagonal with respect to polarization [34]. For the TM contribution, the plane-wave approach allows for the derivation of an exact analytic expression in the more general case of two spheres of arbitrary radii [70]. The previously known result for the plane-sphere geometry [59] is recovered as a particular case.…”
Section: Zero Matsubara Frequencymentioning
confidence: 96%
“…[60] by the multipolar approach. In Section 3.2, we focus on the TE zero-frequency contribution, as the TM correction can be more easily derived from an exact analytical representation obtained either by using bispherical coordinates [59] or by developing the plane-wave basis representation (7) [70].…”
Section: Leading-order Correction For Individual Matsubara Frequenciesmentioning
We consider the Casimir interaction energy between a plane and a sphere of radius R at finite temperature T as a function of the distance of closest approach L. Typical experimental conditions are such that the thermal wavelength λT=ℏc/kBT satisfies the condition L≪λT≪R. We derive the leading correction to the proximity-force approximation valid for such intermediate temperatures by developing the scattering formula in the plane-wave basis. Our analytical result captures the joint effect of the spherical geometry and temperature and is written as a sum of temperature-dependent logarithmic terms. Surprisingly, two of the logarithmic terms arise from the Matsubara zero-frequency contribution.
“…At vanishing frequency, the reflection matrix elements of the sphere are diagonal with respect to polarization [34]. For the TM contribution, the plane-wave approach allows for the derivation of an exact analytic expression in the more general case of two spheres of arbitrary radii [70]. The previously known result for the plane-sphere geometry [59] is recovered as a particular case.…”
Section: Zero Matsubara Frequencymentioning
confidence: 96%
“…[60] by the multipolar approach. In Section 3.2, we focus on the TE zero-frequency contribution, as the TM correction can be more easily derived from an exact analytical representation obtained either by using bispherical coordinates [59] or by developing the plane-wave basis representation (7) [70].…”
Section: Leading-order Correction For Individual Matsubara Frequenciesmentioning
We consider the Casimir interaction energy between a plane and a sphere of radius R at finite temperature T as a function of the distance of closest approach L. Typical experimental conditions are such that the thermal wavelength λT=ℏc/kBT satisfies the condition L≪λT≪R. We derive the leading correction to the proximity-force approximation valid for such intermediate temperatures by developing the scattering formula in the plane-wave basis. Our analytical result captures the joint effect of the spherical geometry and temperature and is written as a sum of temperature-dependent logarithmic terms. Surprisingly, two of the logarithmic terms arise from the Matsubara zero-frequency contribution.
“…For the evaluation of the trace in (5), we adopt the plane-wave basis [28,29]. In view of the geometry of our problem, we decompose the wave vector into a transverse part k with modulus k and a zcomponent which after Wick rotation is written in terms of κ = [ε m (ξ/c) 2 + k 2 ] 1/2 .…”
Section: Scattering Formula For Casimir Interactionmentioning
confidence: 99%
“…In contrast to the scalar case discussed before, we do not have general expressions for the reduced free energy ( 15) and ( 16) for an arbitrary number of round-trips. In the case of two Drude spheres however, an exact expression is known for the sum over the contributions of all round-trips [29]. The difference with respect to the scalar case consists in the absence of the monopolar term associated with = 0 in the reflection matrix element (8) giving rise to the extra term −1 in (11).…”
Section: B Drude Spheres In Vacuum and Dielectric Spheres In Electrolytementioning
confidence: 99%
“…The evaluation of the Gaussian integrals can be mapped onto a combinatorial problem of finding bicolored integer partitions as discussed in detail in Ref. 29. In the end, it turns out that the partitions are related to the elements of the dimensionless capacitance matrix of two spherical conductors.…”
Section: B Drude Spheres In Vacuum and Dielectric Spheres In Electrolytementioning
The electromagnetic Casimir interaction between dielectric objects immersed in salted water includes a universal contribution that is not screened by the solvent and therefore long-ranged. Here, we study the geometry of two parallel dielectric cylinders. We derive the Casimir free energy by using the scattering method. We show that its magnitude largely exceeds the thermal energy scale for a large parameter range. This includes length scales relevant for actin filaments and microtubules in cells. We show that the Casimir free energy is a universal function of the geometry, independent of the dielectric response functions of the cylinders, at all distances of biological interest. While multiple interactions exist between filaments in cells, this universal attractive interaction should have an important role in the cohesion of bundles of parallel filaments.
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