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- W1992045902 abstract "Absorbance difference spectra associated with the light-induced formation of functional states in photosystem II core complexes from Thermosynechococcus elongatus and Synechocystis sp. PCC 6803 (e.g., P(+)Pheo(-),P(+)Q(A)(-),(3)P) are described quantitatively in the framework of exciton theory. In addition, effects are analyzed of site-directed mutations of D1-His(198), the axial ligand of the special-pair chlorophyll P(D1), and D1-Thr(179), an amino-acid residue nearest to the accessory chlorophyll Chl(D1), on the spectral properties of the reaction center pigments. Using pigment transition energies (site energies) determined previously from independent experiments on D1-D2-cytb559 complexes, good agreement between calculated and experimental spectra is obtained. The only difference in site energies of the reaction center pigments in D1-D2-cytb559 and photosystem II core complexes concerns Chl(D1). Compared to isolated reaction centers, the site energy of Chl(D1) is red-shifted by 4 nm and less inhomogeneously distributed in core complexes. The site energies cause primary electron transfer at cryogenic temperatures to be initiated by an excited state that is strongly localized on Chl(D1) rather than from a delocalized state as assumed in the previously described multimer model. This result is consistent with earlier experimental data on special-pair mutants and with our previous calculations on D1-D2-cytb559 complexes. The calculations show that at 5 K the lowest excited state of the reaction center is lower by approximately 10 nm than the low-energy exciton state of the two special-pair chlorophylls P(D1) and P(D2) which form an excitonic dimer. The experimental temperature dependence of the wild-type difference spectra can only be understood in this model if temperature-dependent site energies are assumed for Chl(D1) and P(D1), reducing the above energy gap from 10 to 6 nm upon increasing the temperature from 5 to 300 K. At physiological temperature, there are considerable contributions from all pigments to the equilibrated excited state P*. The contribution of Chl(D1) is twice that of P(D1) at ambient temperature, making it likely that the primary charge separation will be initiated by Chl(D1) under these conditions. The calculations of absorbance difference spectra provide independent evidence that after primary electron transfer the hole stabilizes at P(D1), and that the physiologically dangerous charge recombination triplets, which may form under light stress, equilibrate between Chl(D1) and P(D1)." @default.
- W1992045902 created "2016-06-24" @default.
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- W1992045902 date "2008-07-01" @default.
- W1992045902 modified "2023-10-13" @default.
- W1992045902 title "Spectroscopic Properties of Reaction Center Pigments in Photosystem II Core Complexes: Revision of the Multimer Model" @default.
- W1992045902 cites W1583368715 @default.
- W1992045902 cites W159197400 @default.
- W1992045902 cites W1805686156 @default.
- W1992045902 cites W1960249653 @default.
- W1992045902 cites W1965021206 @default.
- W1992045902 cites W1966604990 @default.
- W1992045902 cites W1967414202 @default.
- W1992045902 cites W1969429591 @default.
- W1992045902 cites W1970401428 @default.
- W1992045902 cites W1972802126 @default.
- W1992045902 cites W1975136195 @default.
- W1992045902 cites W1976314377 @default.
- W1992045902 cites W1977258623 @default.
- W1992045902 cites W1978147444 @default.
- W1992045902 cites W1983840674 @default.
- W1992045902 cites W1987878085 @default.
- W1992045902 cites W1999330901 @default.
- W1992045902 cites W2004177386 @default.
- W1992045902 cites W2004185798 @default.
- W1992045902 cites W2005923041 @default.
- W1992045902 cites W2007276350 @default.
- W1992045902 cites W2011502886 @default.
- W1992045902 cites W2015414343 @default.
- W1992045902 cites W2016517477 @default.
- W1992045902 cites W2021191010 @default.
- W1992045902 cites W2028597160 @default.
- W1992045902 cites W2029606680 @default.
- W1992045902 cites W2029667189 @default.
- W1992045902 cites W2030718784 @default.
- W1992045902 cites W2030852504 @default.
- W1992045902 cites W2032538465 @default.
- W1992045902 cites W2033450625 @default.
- W1992045902 cites W2033655965 @default.
- W1992045902 cites W2035838814 @default.
- W1992045902 cites W2037419497 @default.
- W1992045902 cites W2038015867 @default.
- W1992045902 cites W2044043763 @default.
- W1992045902 cites W2048827175 @default.
- W1992045902 cites W2050965979 @default.
- W1992045902 cites W2053326711 @default.
- W1992045902 cites W2053756131 @default.
- W1992045902 cites W2054529503 @default.
- W1992045902 cites W2056965536 @default.
- W1992045902 cites W2057863409 @default.
- W1992045902 cites W2060234842 @default.
- W1992045902 cites W2067177268 @default.
- W1992045902 cites W2075970495 @default.
- W1992045902 cites W2078350627 @default.
- W1992045902 cites W2079754698 @default.
- W1992045902 cites W2080252029 @default.
- W1992045902 cites W2081363477 @default.
- W1992045902 cites W2081620547 @default.
- W1992045902 cites W2082716445 @default.
- W1992045902 cites W2082722480 @default.
- W1992045902 cites W2083011893 @default.
- W1992045902 cites W2083907491 @default.
- W1992045902 cites W2087069790 @default.
- W1992045902 cites W2093386549 @default.
- W1992045902 cites W2102023258 @default.
- W1992045902 cites W2105312299 @default.
- W1992045902 cites W2108168954 @default.
- W1992045902 cites W2122008044 @default.
- W1992045902 cites W2126285505 @default.
- W1992045902 cites W2132719679 @default.
- W1992045902 cites W2134246362 @default.
- W1992045902 cites W2152513820 @default.
- W1992045902 cites W2154680016 @default.
- W1992045902 cites W2155060745 @default.
- W1992045902 cites W2160672315 @default.
- W1992045902 cites W2165874911 @default.
- W1992045902 cites W2172097389 @default.
- W1992045902 doi "https://doi.org/10.1529/biophysj.107.123935" @default.
- W1992045902 hasPubMedCentralId "https://www.ncbi.nlm.nih.gov/pmc/articles/2426664" @default.
- W1992045902 hasPubMedId "https://pubmed.ncbi.nlm.nih.gov/18339736" @default.
- W1992045902 hasPublicationYear "2008" @default.
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