Mr. Razeghifard et al., In vivo, in vitro, and calculated vibrational spectra of plastoquinone andthe plastosemiquinone anion radical, J PHYS CH B, 103(44), 1999, pp. 9790-9800
Plastoquinone (PQ-9) is active as an electron/proton transfer component in
photosynthetic membranes. For example, in the photosynthetic complex, photo
system II (PSII), PQ-9 acts as Q(A), a one-electron acceptor, and as Q(B),
a two electron, two proton accepting species. Light-minus-dark difference F
ourier transform infrared (FT-IR) spectroscopy is a technique with which me
chanistic information can be obtained concerning PSII. Here, we present com
bined experimental and computational studies designed to identify the vibra
tional contributions of the electron acceptor, Q(A), in its oxidized and on
e-electron reduced states to the difference FT-TR spectrum. Infrared spectr
a of decyl-PQ and PQ-9 were obtained; the difference infrared spectra assoc
iated with the formation of the corresponding anion radicals were also gene
rated in ethanol solutions. Vibrational mode assignments were made based on
hybrid Hartree-Fock/density functional (HF/DF) B3LYP calculations with a 6
-31G(d) basis set. Calculations were performed for hydrogen bonded models o
f PQ-1 and its radical anion. In addition, a methionine-tolerant strain of
the cyanobacterium, Synechocystis sp. PCC 6803, was used to deuterate PQ-9
in PSII. The macrocycle and phytol tail of chlorophyll were not labeled by
this procedure. Mass spectral data may be consistent with pal-tial 13(3) me
thoxy labeling of chlorophyll, Lack of phytol labeling implies that caroten
oids were unlabeled. Difference FT-IR spectra were then obtained by illumin
ation at 80 K, resulting in the one-electron reduction of Q(A). When spectr
a were obtained of PSII preparations, in which 39% of PQ was H-2(3) labeled
and 48% was H-2(6) labeled, isotope-induced shifts were observed. Comparis
on of these data to vibrational spectra obtained in vitro and to mode frequ
encies and intensities from B3LYP/6-31G(d) calculations provides the basis
for vibrational mode assignments.