Electron spin polarization in consecutive spin-correlated radical pairs: Application to short-lived and long-lived precursors in type 1 photosynthetic reaction centres
Ye. Kandrashkin et al., Electron spin polarization in consecutive spin-correlated radical pairs: Application to short-lived and long-lived precursors in type 1 photosynthetic reaction centres, APPL MAGN R, 15(3-4), 1998, pp. 417-447
An analytical treatment of the spin dynamics in sequential photoinduced cor
related coupled radical pairs is presented and applied to the spectra of th
e states P(+)A(1)(-) and P+FX- in type 1 photosynthetic reaction centres. E
xpressions for the spin polarized spectra are derived for the specific limi
ting cases of a very short-lived and very long-lived primary radical pair w
hich correspond to the situation found in heliobacteria and photosystem I (
PSI), respectively. The inhomogeneous line-broadening due to the unresolved
hyperfine couplings is taken explicitly into account. It is shown that the
density matrix of the secondary pair rho(2) can be written as the sum of t
wo terms corresponding to (i) the part which is independent of the spin dyn
amics in the precursor, (ii) the additional spin polarization which is gene
rated during the, lifetime of the precursor and transferred to the secondar
y pair. The latter term contains two contributions which arise from the dif
ference of the Zeeman interactions of the radicals in the primary pair and
from the inhomogeneous line broadening. The predicted polarization patterns
are compared to those established for chemically induced dynamic electron
polarization (CIDEP) when uncoupled radicals are generated from a radical p
air precursor. The expressions are then used to simulate the experimental s
pectra of the consecutive pairs PCA; and P+FX- in PSI using parameters deri
ved entirely from independent experimental data. Excellent agreement with t
he experimental results is obtained. The spectra of P+FX- in heliobacteria
at X- and K-band are also simulated and it is shown that the observed polar
ization patterns can be reproduced assuming direct electron transfer from A
(0) to F-X with a time constant of tau = 600 ps.