2013
DOI: 10.1103/physreva.87.062105
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Dispersion forces inside metallic waveguides

Abstract: We consider the dispersion energy of a pair of dipoles embedded in a metallic waveguide with transverse dimension $a$ smaller than the characteristic dipolar wavelength. We find that $a$ sets the scale that separates retarded, Casimir-Polder-like, from quasistatic, van der Waals-like, interactions. Whereas in the retarded regime, the energy decays exponentially with inter-dipolar distance, typical of evanescent waves, in the van der Waals regime, the known free-space result is obtained. This short-range scalin… Show more

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Cited by 54 publications
(90 citation statements)
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References 21 publications
(31 reference statements)
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“…For the same geometry, an exponential decay was also found at any finite temperature [23]. An exponential reduction of the interaction between the atoms has been also observed when they are confined in a rectangular waveguide and their distance is large compared to the diameter of the waveguide [26]. Contrary to that, a recent study of two atoms placed inside a transmission line consisting of two concentric metallic cylinders demonstrated a huge amplification of the interaction between the atoms due to the one-dimensional character of propagating fluctuations in this geometry [27].…”
Section: Discussionmentioning
confidence: 57%
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“…For the same geometry, an exponential decay was also found at any finite temperature [23]. An exponential reduction of the interaction between the atoms has been also observed when they are confined in a rectangular waveguide and their distance is large compared to the diameter of the waveguide [26]. Contrary to that, a recent study of two atoms placed inside a transmission line consisting of two concentric metallic cylinders demonstrated a huge amplification of the interaction between the atoms due to the one-dimensional character of propagating fluctuations in this geometry [27].…”
Section: Discussionmentioning
confidence: 57%
“…Clearly, all modes in our cylindrical shell, and also in the rectangular waveguide of Ref. [26] are massive, explaining an exponential reduction of the interaction. However, for two parallel conducting plates, there exists a massless mode only for TM polarization [32].…”
Section: Discussionmentioning
confidence: 99%
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“…To this end we shall use the results of the weak-coupling, non-Markovian master equation [18,27,28], whereby…”
Section: System-bath Decorrelation Via Qnd Measurementsmentioning
confidence: 99%
“…Refs. [44][45][46][47][48]). (2) What is the optimal scheduling (cycle form) for attaining the best performance: reciprocating, continuous or possibly some intermediate (hybrid) cycles?…”
Section: Introductionmentioning
confidence: 99%