1993
DOI: 10.1016/0014-5793(93)80837-k
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Similarity of primary radical pair recombination in photosystem II and bacterial reaction centers

Abstract: We report temperature and magnetic field dependent measurements of the recombination dynamics of the radical pair P680+Pheo-in D,D,cytbSSg reaction centers of photosystem II and compare the results to those obtained in bacterial reaction centers. In photosystem II the rate of recombination to the groundstate is found to be slower than in the bacterial reaction centers by a factor of at least 50. This difference arises from the different redox potentials of the pigments of plant and bacterial reaction centers. … Show more

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Cited by 45 publications
(30 citation statements)
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“…The long-lived component is readily assigned to be mainly due to the radical pair state P680 ϩ Pheo. This state has been reported to have a lifetime of tens of nanoseconds at low temperature (35,36), and its spectrum at 240 K is very similar to that reported earlier at RT by Klug et al (ref. 22 and references therein).…”
Section: Discussionsupporting
confidence: 72%
“…The long-lived component is readily assigned to be mainly due to the radical pair state P680 ϩ Pheo. This state has been reported to have a lifetime of tens of nanoseconds at low temperature (35,36), and its spectrum at 240 K is very similar to that reported earlier at RT by Klug et al (ref. 22 and references therein).…”
Section: Discussionsupporting
confidence: 72%
“…In this case the probability for 3 Chl formation could be very small (18,40). In terms of triplet formation efficiency, one may consider the following series: [P 680 •…”
Section: Discussionmentioning
confidence: 99%
“…•ϩ ͞Pheo •Ϫ may be regenerated in the dark and charge recombination may result in the triplet chlorophyll ( 3 Chl) formation (17,18). Therefore one would expect that charge recombination and hence damage to PSII will occur with increased efficiency per photon absorbed as the rate of excitation decreases.…”
mentioning
confidence: 99%
“…b The sum of the rate constants for radiative (fluorescence) and non-radiative excited-state decay is assumed to be 1 ns 21 for the here used PSII membrane particles (Leibl et al 1989). c Rate constant for decay of the P680 1 Phe 2 triplet state from (Volk et al 1993). d Population of the P680 1 Phe 2 and excited-antenna state, respectively, relative to the P680 1 Q 2 A population [¼exp(2DG i /k B T)].…”
Section: Quantum Yield Of Individual Recombination Loss Pathwaysmentioning
confidence: 99%