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^6
ð 9 : 1 Þ
where 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 0
S 1
Donor
Acceptor
Energy-matched
donor/acceptor
transitions
Acceptor
excitation
transitions
Non-radiative
transitions
Acceptor
fluorescence
transitions
Donor
excitation
transitions
Donor
fluorescence
transitions
Fig. 9.4 State transitions in a FRET process
Normalized intensity
Wavelength (arbitrary units)
Donor
absorption
Donor
emission
Acceptor
absorption
Acceptor
emission
Donor/acceptor
spectral overlap
Fig. 9.5 Absorption and emission spectra of the donor and acceptorfluorophores
9.2 FRET/FLIM 265