You have requested a machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Neither SPIE nor the owners and publishers of the content make, and they explicitly disclaim, any express or implied representations or warranties of any kind, including, without limitation, representations and warranties as to the functionality of the translation feature or the accuracy or completeness of the translations.
Translations are not retained in our system. Your use of this feature and the translations is subject to all use restrictions contained in the Terms and Conditions of Use of the SPIE website.
Chapter 14: Resonance Energy Transfer: Theoretical Foundations and Developing Applications
Access to the requested content is limited to institutions that have purchased or subscribe to SPIE eBooks.
You are receiving this notice because your organization may not have SPIE eBooks access.*
*Shibboleth/Open Athens users─please
sign in
to access your institution's subscriptions.
To obtain this item, you may purchase the complete book in print format on
SPIE.org.
Abstract
In the wide range of materials that are characterised by broad, relatively featureless optical spectra, the absorption of light in the ultraviolet-visible wavelength region is typically followed by rapid internal processes of dissipation and degradation of the acquired energy, the latter ultimately to be manifest in the form of heat. In more complex materialsâthose comprising a variety of light-absorbing atomic or molecular components (chromophores) with optically well characterised absorption and fluorescence bandsâthe absorption of light is commonly followed by a spatial translation of the absorbed electromagnetic radiation between different, though usually closely separated, chromophores. The process takes place well before the completion of any thermal degradation in such materials. This primary relocation of the acquired electronic energy, immediately following photo-excitation, is accomplished by a mechanism that has become known as resonance energy transfer (RET). (At an earlier stage in the development of these ideas, the term "resonance" was used to signify that no molecular vibrations were excited; however, such usage is now known to be relevant to few systems and has largely fallen into abeyance.) An alternative designation for the process is electronic energy transfer (EET); both terms are widely used, and in each case, the first letter of the acronym serves as a distinction from electron transfer.
In complex multichromophore materials, the singular properties of RET allow the flow of energy to exhibit a directed character. Because the process operates most efficiently between near-neighbor chromophores, the resonance propagation of energy through such a system generally takes the form of a series of short steps; an alternative process involving fewer long steps proves considerably less favourable. In suitably designed materials, the pattern of energy flow following optical absorption is thus determined by a sequence of transfer steps, beginning and ending at chromophores that differ chemically, or, if the chromophores are structurally equivalent, through local modifications in energy level structure reflecting the influence of their electronic environment. Hence, individual chromophores that act in the capacity of excitation acceptors can subsequently adopt the role of donors. This effect contributes to a crucial, property-determining characteristic for the channeling of electronic excitation in photosynthetic systems; the same principles are emulated in synthetic energy harvesting systems such as the fractal polymers known as dendrimers.
Online access to SPIE eBooks is limited to subscribing institutions.