2016
DOI: 10.1088/0143-0807/37/3/034001
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Quantum optical dipole radiation fields

Abstract: We introduce quantum optical dipole radiation fields defined in terms of photon creation and annihilation operators. These fields are identified through their spatial dependence, as the components of the total fields that survive infinitely far from the dipole source. We use these radiation fields to perturbatively evaluate the electromagnetic radiated energy-flux of the excited dipole. Our results indicate that the standard interpretation of a bare atom surrounded by a localised virtual photon cloud, is diffi… Show more

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Cited by 8 publications
(11 citation statements)
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References 36 publications
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“…Our aim is to identify the contribution made by the quantum vacuum, and in particular, the role played by vacuum source-field interference. The treatment in this section extends previous perturbative treatments found in [21,28,29,32].…”
Section: Vacuum-source Correlations and Radiation Intensitysupporting
confidence: 67%
See 1 more Smart Citation
“…Our aim is to identify the contribution made by the quantum vacuum, and in particular, the role played by vacuum source-field interference. The treatment in this section extends previous perturbative treatments found in [21,28,29,32].…”
Section: Vacuum-source Correlations and Radiation Intensitysupporting
confidence: 67%
“…We now turn our attention to the contribution of vacuum source-correlations to the radiation intensity. In references [21,28,29,32] Eq. ( 27) is used to perturbatively calculate the radiated power.…”
Section: Vacuum Source-field Correlationsmentioning
confidence: 99%
“…The (α, k M )-gauge vector potential is within the EDA (93) such that A 1 (0) = 0 is recovered in the limit k M → ∞. More generally, vanishing of A 1M (r) to dipole order requires that ÃT (k) ≈ 0 for k ≥ k M .…”
Section: H Sharing Out the Constrained Degrees Of Freedommentioning
confidence: 99%
“…In order to understand the interplay between localfields, virtual processes, and subsystem gauge-relativity, we now consider various energy-densities in the vicinity of a dipole [17,28,29,45,[54][55][56][57][89][90][91][92][93]. In finding energydensities different methods are available and are suitable for different purposes.…”
Section: Second-order Energy-densitiesmentioning
confidence: 99%
“…At this stage, it becomes important to return to the generalized matrix elements M FI to distinguish expectation values (signifying identical initial and final system states) from the off-diagonal matrix elements that feature as modulus squares in process observables. The distinction, recently re-emphasized by Stokes [82], becomes especially important when physically identifiable effects arise from the interference between terms involving different kinds of multipolar coupling-chiral and mechanical effects in particular, as shown in other recent work [83][84][85] To secure an expression for the rate of an observable transition process, we now work from Equation (13) to arrive at the following:…”
Section: Observablesmentioning
confidence: 99%