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W W Parson

Publications and source records attributed to W W Parson.

At least 55 records · Page 3Linked to original sources

Delayed fluorescence from Rhodopseudomonas sphaeroides following single flashes.

Delayed fluorescence from Rhodopseudomonas sphaeroides chromatophores was studied with the use of short flashes for excitation. Although the delayed fluorescence probably arises from a back-reaction between the oxidized reaction center bacteriochlorophyll complex (P+) and the reduced electron acceptor (X-), the decay of delayed fluorescence after a flash is much faster (tau1/2 approximately 120 mus) than the decay of P+X-. The rapid decay of delayed fluorescence is not due to the uptake of a proton from the solution, nor to a change in membrane potential. It correlates with small optical absorbance changes at 450 and 770 nm which could reflect a change in the state of X-. The intensity of the delayed fluorescence is 11-18-fold greater if the excitation flashes are spaced 2 s apart than it is if they are 30 s apart. The enhancement of delayed fluorescence at high flash repetition rates occurs only at redox potentials which are low enough (less than +240 mV) so that electron donors are available to reduce P+X- to PX- in part of the reaction center population. The enhancement decays between flashes as PX- is reoxidized to PX, as measured by the recovery of photochemical activity. Evidently, the reduction of P+X- to PX- leads to the storage of free energy that can be used on a subsequent flash to promote delayed fluorescence. The reduction of P+X- also is associated with a carotenoid spectral shift which decays as PX- is reoxidized to PX. Although this suggests that the free energy which supports the delayed fluorescence might be stored as a membrane potential, the ionophore gramicidin D only partially inhibits the enhancement of delayed fluorescence. With widely separated flashes, gramicidin has no effect on delayed fluorescence. At redox potentials low enough to keep X fully reduced, delayed fluorescence of the type described above does not occur, but one can detect weak luminescence which probably is due to phosphorescence of a protoporphyrin.

Bacteriochlorophylls↗

The type, amount, location, and energy transfer properties of the carotenoid in reaction centers from Rhodopseudomonas sphaeroides.

Analysis of photosynthetic reaction centers from Rhodopseudomonas sphaeroides strains 2.4.1 and Ga shows that each contains approx. 1 mol of a specific carotenoid per mol of reaction center. In strain 2.4.1. the carotenoid is spheroidene (1-methoxy-3,4-didehydro-1,2,7',8',-tetrahydro-psi,psi-carotene); in strain Ga, it is chloroxanthin (1-hydroxy-1, 2, 7', 8'-tetrahydro-psi,psi-carotene). The carotenoid is bound to the same pair of proteins as are the bacteriochlorophylls and bacteriopheophytins of the reaction center. This binding induces strong circular dichroism in the absorption bands of the carotenoid. The carotenoid is close enough to the other pigments of the reaction center so that light energy transfers efficiently from the carotenoid to the bacteriochlorophyll, sensitizing bacteriochlorophyll fluorescence. The fluorescence polarization spectrum of the reaction centers shows that the transition vectors for the visible absorption bands of the carotenoid lie approximately parallel to the 600 nm (Qx) transition of the bacteriochlorophyll complex.

Carotenoids↗

Carotenoid triplet states in reaction centers from Rhodopseudomonas sphaeroides and Rhodospirillum rubrum.

Purified photochemical reaction centers from three strains of Rhodopseudomonas sphaeroides and two of Rhodospirillium rubrum were reduced with Na2S2O4 so as to block their photochemical electron transfer reactions. They then were excited with flashes lasting 5-30 ns. In all cases, absorbance measurements showed that the flash caused the immediate formation of a transient state (PF) which had been detected previously in reaction centers from Rps. sphaeroides strain R26. Previous work has shown that state PF is an intermediate in the photochemical electron transfer reaction in the reaction centers of that particular strain, and the present work generalizes that conclusion. In the reaction centers from two strains that lack carotenoids (Rps. sphaeroides R26 and R. rubrum G9), the decay of PF yields a longer-lived state (PR) which is probably a triplet state of the bacteriochlorophyll of the reaction center. In the R26 preparation, the decay of PF was found to have a half-time of 10 +/- 2 ns. The decay kinetics rule out the identification of PF as the fluorescent excited singlet state of the reaction center. In the reaction centers from three strains that contain carotenoids (Rps sphaeroides 2.4.1 and Ga, and R. rubrum S1), state PR was not detected, and the decay of PF generated triplet states of carotenoids. The efficiency of the coupling between the decay of PF and the formation of the carotenoid triplet appeared to be close to 100% at room temperature, but somewhat lower at 77 degrees K. Taken with previous results, this suggests that the coupling is direct and does not require the intermediate formation of state PR. This conclusion would be consistent with the view that PF is a biradical which can be triplet in character.

Carotenoids↗

Delayed fluorescence from Rhodopseudomonas viridis following single flashes.

Delayed fluorescence from Rhodopseudomonas viridis membrane fragments has been studies using a phosphoroscope employing single, short actinic flashes, under conditions of controlled redox potential and temperature. The emission spectrum shows that delayed fluorescence is emitted by the bulk, antenna bacteriochlorophyll. The energy for delayed fluorescence, however, must be stored in a reaction-center complex including the photooxidized form (P+) of the primary electron-donor (P) and the photoreduced form (X MINUS) of the primary electron-acceptor. This is shown by the following observations: (1) Delayed luminescence is quenched (a) at low redox potentials which allow cytochromes to reduce P+ rapidly after the flash, (b) at higher redox potentials which, by oxidizing P chemically, prevent the photochemical formation of P+X minus, and (c) upon transfer of an electron from X minus to a secondary acceptor, Y. (2) Under conditions that prevent the reduction of P+ by cytochromes and the oxidation of X minus by Y, the decay kinetics of delayed fluorescence are identical with those of P+X minus, as measured from optical absorbance changes. The main decay route for P+X minus under these conditions has a rate-constant of approximately 10-3-s-minus 1. In contrase, a comparison of the intensities of delayed and prompt fluorescence indicates that the process in which P+X minus returns energy to the bulk bacteriochlorophyll has a rate-constant of 3.7 s-minus 1, at 295 degrees K and pH 7.8. The decay kinetics of P+X minus and delayed fluorescence change little with temperature, whereas the intensity of delayed fluorescence increases with increasing temperature, having an activation energy of 12.5 kcal mol-mol- minus 1. We conclude that the main decay route involves tunneling of an electron from X minus to P+, without the promotion of P to an excited state. Delayed fluorescence requires such a promotion, followed by transfer of energy to the bulk bacteriochlorophyll, and this combination of events is rare. The activation energy, taken with potentiometric data, indicates that the photochemical conversion of PX to P+X minus results in increases of both the energy and the entropy of the system, by 16.6 kcal-mol- minus 1 and 8.8 cal-mol- minus 1-deg- minus 1. The intensity of delayed fluorescence depends strongly on the pH; the origin of this effect remains unclear.

Calorimetry↗

Excited states of photosynthetic reaction centers at low recox potentials.

In preparations of photochemical reaction centers from Rhodopseudomonas spheroides R-26, lowering the recox potential so as to reduce the primary electron acceptor prevents the photochemical transfer of an electron from bacteriochlorophyll to the acceptor. Measuring absorbance changes under these conditions, we found that a 20-ns actinic flash converts the reaction center to a new state, P-F, which then decays with a half-time that is between 1 and 10 ns at 295 degrees K. At 25 degrees K, the decay half-time is approx. 20 ns. The quantum yield of state P-F appears to be near 1.0, both at 295 and at 15 degrees K. State P-F could be an intermediate in the photochemical electron-transfer reaction which occurs when the acceptor is in the oxidized form. Following the decay of state P-F, we detected another state, P-R, with a decay half-time of 6 mus at 295 degrees K and 120 mus at 15 degrees K. The quantum yield of state P-R is approx. 0.1 at 295 degrees K, but rises to a value nearer 1.0 at 15 degrees K. The kinetics and quantum yields are consistent with the view that state P-R forms from P-F. State P-R seems likely to be a side-product, rather than an intermediate in the electron-transfer process. The decay kinetics indicate that state P-F cannot be identical with the lowest excited singlet state of the reaction center. One of the two states, P-F or P-R, probably is the lowest excited triplet state of the reaction center, but it remains unclear which one.

Chlorophyll↗

Picosecond detection of an intermediate in the photochemical reaction of bacterial photosynthesis.

Preparations of photosynthetic reaction centers from Rhodopseudomonas sphaeroides were excited with flashes lasting approximately 8 psec. Immediately after the excitation, there appeared a transient state which was characterized by new absorption bands near 500 and 680 nm, by a bleaching of bands near 540, 600, 760, and 870 nm, and by a blue shift of a band near 800 nm. The transient state decayed with an exponential decay time,t, of 246 plus or minus 16 psec after the flash. As the transient state decayed, the radical cation of the reaction center bacteriochlorophyll complex appeared. This indicates that the transient state is an intermediate in the photooxidation of the bacteriochlorophyll. The absorpiton spectrum of the transient state shows the state to be identical with a state (P-F) which has been detected previously in reaction centers that are prevented from completing the photooxidation, because of chemical reduction of the electron acceptor. Analysis of the spectrum suggests that the formation of P-F involves electron transfer from one bacteriochlorophyll molecule to another within the reaction center, or possibly from bacteriochlorophyll to the bacteriopheophytin of the complex. The initial absorbance changes after flash excitation also include a bleaching of an absorption band at 800 nm. The bleaching decays with tau approximately equal to 30 pse. The bleaching appers not to be a secondary effect, but rather to revael another early step in the primary photochemical reaction.

Bacteriochlorophylls↗