area indicates the overlap between the donor emission and the acceptor excitation
spectra.
The efficiency E of the energy transfer is given by the Förster relation
E¼
R^60
R^60 þR^6ð 9 : 1 Þwhere the Förster distance R 0 is thefluorophore separation at which 50 % of the
energy is transferred and R is the actual distance between thefluorophores. Thus,
because the energy transfer efficiency is inversely proportional to the sixth power of
the distance between the donor and the acceptor, the FRET process is extremely
sensitive to small changes in the separations of the donor and acceptorfluorophores
(see Example9.2and Prob. 9.3). In FRET applications the experimental separation
distances typically are on the order of the Förster distance.
S 0S 1DonorAcceptorEnergy-matched
donor/acceptor
transitionsAcceptor
excitation
transitionsNon-radiative
transitionsAcceptor
fluorescence
transitionsDonor
excitation
transitionsDonor
fluorescence
transitionsFig. 9.4 State transitions in a FRET process
Normalized intensityWavelength (arbitrary units)Donor
absorptionDonor
emissionAcceptor
absorptionAcceptor
emissionDonor/acceptor
spectral overlapFig. 9.5 Absorption and emission spectra of the donor and acceptorfluorophores
9.2 FRET/FLIM 265