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Biophys J, July 2001, p. 538-546, Vol. 81, No. 1


*Faculty of Sciences, Department of Physics and Astronomy, Vrije
Universiteit Amsterdam, 1081 HV Amsterdam, The Netherlands; and
Debye Institute, Utrecht University, 3508 TA Utrecht, The
Netherlands
Two-photon excitation, time-resolved fluorescence
microscopy was used to investigate the fluorescence quenching
mechanisms in aggregates of light-harvesting chlorophyll
a/b pigment protein complexes of
photosystem II from green plants (LHCII). Time-gated microscopy images
show the presence of large heterogeneity in fluorescence lifetimes not
only for different LHCII aggregates, but also within a single
aggregate. Thus, the fluorescence decay traces obtained from
macroscopic measurements reflect an average over a large distribution
of local fluorescence kinetics. This opens the possibility to resolve
spatially different structural/functional units in chloroplasts and
other heterogeneous photosynthetic systems in vivo, and gives the
opportunity to investigate individually the excited states dynamics of
each unit. We show that the lifetime distribution is sensitive to the
concentration of quenchers contained in the system. Triplets, which are
generated at high pulse repetition rates of excitation (>1 MHz),
preferentially quench domains with initially shorter fluorescence
lifetimes. This proves our previous prediction from singlet-singlet
annihilation investigations (Barzda, V., V. Gulbinas, R. Kananavicius,
V. Cervinskas, H. van Amerongen, R. van Grondelle, and L. Valkunas.
2001. Biophys. J. 80:2409-2421) that shorter
fluorescence lifetimes originate from larger domains in LHCII
aggregates. We found that singlet-singlet annihilation has a strong
effect in time-resolved fluorescence microscopy of connective systems
and has to be taken into consideration. Despite that, clear differences
in fluorescence decays can be detected that can also qualitatively be understood.
Biophys J, July 2001, p. 538-546, Vol. 81, No. 1
© 2001 by the Biophysical Society 0006-3495/01/07/538/09 $2.00
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