2008
DOI: 10.1139/v08-099
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Mechanistic principles and applications of resonance energy transfer

Abstract: Abstract:Resonance energy transfer is the primary mechanism for the migration of electronic excitation in the condensed phase. Well-known in the particular context of molecular photochemistry, it is a phenomenon whose much wider prevalence in both natural and synthetic materials has only slowly been appreciated, and for which the fundamental theory and understanding have witnessed major advances in recent years. With the growing to maturity of a robust theoretical foundation, the latest developments have led t… Show more

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Cited by 51 publications
(48 citation statements)
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References 103 publications
(128 reference statements)
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“…With the development of a robust theory rigorously based on quantum electrodynamics [3], it has become possible to encompass a complete photon history as an embodiment of the causal linkage between source decay and detector excitation events [4]. In the QED representation, the propagation of light from an emissive source to an absorptive detector is the long-range limit of a general mechanism that, when it operates over subwavelength distances, is usually designated resonance energy transfer [5].…”
Section: Foundation Theorymentioning
confidence: 99%
“…With the development of a robust theory rigorously based on quantum electrodynamics [3], it has become possible to encompass a complete photon history as an embodiment of the causal linkage between source decay and detector excitation events [4]. In the QED representation, the propagation of light from an emissive source to an absorptive detector is the long-range limit of a general mechanism that, when it operates over subwavelength distances, is usually designated resonance energy transfer [5].…”
Section: Foundation Theorymentioning
confidence: 99%
“…[46][47][48] As with the optically induced pair forces, the throughput radiation once again emerges in a final state that is unchanged from its initial state, while in this case the material system experiences a transfer of energy from A to B. Thus, for the initial and final states of the system as a whole we have ͉I͘ = ͉A ␣ ,B 0 ;n͑p,l͒͘, ͉F͘ = ͉A 0 ,B ␤ ;n͑p,l͒͘.…”
Section: Laser-assisted Resonance Energy Transfermentioning
confidence: 99%
“…For present purposes, equation (1) can be regarded as being applied to a system comprising just two material components, ξ signifying the source/donor or the detector/acceptor. By inspection of this expression it is immediately apparent that, in contrast to most classical descriptions, energy transfer is not mediated by instantaneous coupling interactions-note the absence of any terms connecting different chromophores-but causally, through an electromagnetic field with a finite speed of propagation [21]. The term of most interest in equation (1) is the interaction term, since the light-matter interactions act as a perturbation to the total energy of the particles and the fields in isolation.…”
Section: Radial Distribution Of the Field From An Electric Dipolementioning
confidence: 99%