TRANSFER OF EXCITATION-ENERGY IN A 3-DIMENSIONAL-DOPED MOLECULAR-CRYSTAL .5. SELF-CONSISTENCY OF THE TEMPORAL PROCESSES INVOLVED IN ENERGY-TRANSFER IN PHOTOSYNTHETIC UNITS
Sn. Datta et al., TRANSFER OF EXCITATION-ENERGY IN A 3-DIMENSIONAL-DOPED MOLECULAR-CRYSTAL .5. SELF-CONSISTENCY OF THE TEMPORAL PROCESSES INVOLVED IN ENERGY-TRANSFER IN PHOTOSYNTHETIC UNITS, International journal of quantum chemistry, 60(5), 1996, pp. 1045-1055
Numerical experiments were carried out to determine the timewise self-
consistency of different physical processes involved in the energy tra
nsfer in green plant photosynthetic units. A 6 x 6 x 6 array of chloro
phyll-a with cubic lattice constants a = b = c = 20 Angstrom was chose
n as a model of the thylakoid disc. Another model aggregate was obtain
ed by substituting chlorophyll-b molecules for some of the chlorophyll
-a molecules. In both models, a reaction center occupied a central sit
e in the last xy plane. Two extreme arrangements were considered for t
he orientation of molecules. In one, the transition moments of all mol
ecules were directed along the y-axis. The other had chlorophyll molec
ules randomly oriented. The four resulting model systems were used in
our investigation on exciton generation, transport, decay by fluoresce
nce, and trapping. All excitons were assumed to be generated by a 20 m
s exposure to sunlight at high altitudes. The general trends noticed f
rom these computations are as follows: The number of excitons generate
d is influenced by lattice disorders. Disorders also increase the time
for the establishment of an equilibrium distribution The decay of exc
itons by fluorescence is always a monotonic function of time. The ener
gy transfer is adversely affected by a lower degree of orientation in
the crystal: The trapping time increases with disorder. The number of
trappings decreases with the onset of fluorescence of the host molecul
es and the trap. From these investigations, we also made three specifi
c observations: (1) The efficiency of exciton utilization varies from
12% for a completely random arrangement of transition dipoles to 46% f
or a perfectly ordered arrangement. This agrees with the experimental
efficiency, about 20%. (2) The number of excitons trapped varies from
one to six. This tallies with the time scale of electron transfer alon
g the Z-scheme that requires at least two excitons trapped in about 20
ms. Thus, the photon density and the exciton transfer rate are consis
tent with the rates of electron transfers. (3) The trapping rate also
indicates that the thylakoid disc must resemble a considerably ordered
system. (C) 1996 John Wiley & Sons, Inc.