Computer simulation of the exciton transfer in the coupled ring antenna subunits of bacteria photosynthetic systems

Citation
P. Herman et I. Barvik, Computer simulation of the exciton transfer in the coupled ring antenna subunits of bacteria photosynthetic systems, J PHYS CH B, 103(49), 1999, pp. 10892-10909
Citations number
72
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
JOURNAL OF PHYSICAL CHEMISTRY B
ISSN journal
15206106 → ACNP
Volume
103
Issue
49
Year of publication
1999
Pages
10892 - 10909
Database
ISI
SICI code
1520-6106(199912)103:49<10892:CSOTET>2.0.ZU;2-I
Abstract
A common accepted feature of the purple bacteria antenna systems seems to b e a ring structure of their subunits LH2 and LH1. We concentrate our invest igation on a delivery time of the energy through the subunits LH2 and LH1 o f the antenna system to the reaction center. We are dealing with a model sy stem consisting of one ring LH2 and one ring LH1. We have used structure da ta from Rhodopseudomonas acidophila. We investigate the exciton transfer in side and between LH2 and LH1 rings in the presence of the interaction with a bath. One can expect the incoherent (hopping) regime of the exciton trans fer among the LH2 and LH1 rings. The exciton transfer inside the rings LH2 and LH1 is treated in a quasicoherent regime. One is therefore forced to de al with the time development of the full exciton density matrix of the exci ton to take into account phase relations given by off-diagonal elements, co mpleting in such a way information given by the site occupation probabiliti es P-m(t), diagonal elements of the exciton density matrix. Time dependence of the exciton density matrix is governed by dynamic equations which form an extension of the stochastic Liouville equation method with a Haken-Strob l-Reineker parametrization. Some known shortcomings of the original HSR-SLE treatment are removed in our model: (a) we replace a classical stochastic field by a quantum field and (b) we introduce a new parameter A to provide a correct imbalance among the extended states at finite temperatures for lo ng times due to energy relaxation. We discuss the influence of a local ener gy and a transfer integral heterogeneity, distance, and orientation depende nce of the transfer rates between rings, relaxation, etc., on the energy de livery time.