2015
DOI: 10.1103/physreva.91.052707
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Modified and controllable dispersion interaction in a one-dimensional waveguide geometry

Abstract: Dispersion interactions such as the van derWaals interaction between atoms or molecules derive from quantum fluctuations of the electromagnetic field and can be understood as the exchange of virtual photons between the interacting partners. Any modification of the environment in which those photons propagate will thus invariably lead to an alteration of the van der Waals interaction. Here we show how the two-body dispersion interaction inside a cylindrical waveguide can be made to decay asymptotically exponent… Show more

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Cited by 23 publications
(49 citation statements)
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“…In addition, both the oscillating and monotonous force components are expected to arise in waveguides as recently studied in Refs. [33][34][35][36]. It could be also interesting to generalize our model to include finite temperature, by chancing the fluctuation relations of the electromagnetic field, and to consider many-body vdW forces.…”
Section: Discussionmentioning
confidence: 99%
“…In addition, both the oscillating and monotonous force components are expected to arise in waveguides as recently studied in Refs. [33][34][35][36]. It could be also interesting to generalize our model to include finite temperature, by chancing the fluctuation relations of the electromagnetic field, and to consider many-body vdW forces.…”
Section: Discussionmentioning
confidence: 99%
“…Hence if we know the handedness of one chiral molecule we are able to determine the handedness of the other one with this experiment. Note that the recently predicted exponential suppression of the electric vdW potential in a parallel mirror cavity [36] or in a planar waveguide [37] might further assist the observability of the chiral component. Three-body discriminatory chiral contributions are also present in the cavity configuration, however they are smaller with respect to the analyzed two-body contributions.…”
mentioning
confidence: 99%
“…Here, interactions are mediated by the guided mode with wave number k = 2π/λ and [40,41] and multiple coherent scattering affects the system properties. For even N and Bragg or anti-Bragg conditions (odd or even 2L/λ ∈ N, respectively), A −1 can be exactly diagonalized by a Fourier ansatz (cf.…”
Section: Collective States Multiple Scattering and A Phase Diagrammentioning
confidence: 99%