Light-induced absorbance changes due to Photosystems 1 and 2 in spinach chloroplasts at −50 °C

Absorbance changes in the region 500–565 nm and at 702 nm, brought about by excitation of Photosystems 1 and 2, respectively, were measured in spinach chloroplasts at ?50 °C. Either dark-adapted chloroplasts were used or chloroplasts preilluminated with a number of short saturating flashes just before cooling.Both photosystems were found to cause a light-induced increase of absorbance at 518 nm (due to “P518”). The System 1-induced change was not affected by preillumination. It decayed within 1 s in the dark and showed similar kinetics as P700. Experiments in the presence of external electron acceptors (methylviologen or Fe(CN)₆^3?) suggested that P518 was not affected by the redox state of the primary electron acceptor of System 1. The absorbance increase at 518 nm due to System 2 decayed in the dark with a half-time of several min. The kinetics were similar to those of C-550, the presumed indicator of the primary electron acceptor of System 2. After two flashes preillumination the changes due to P518 and C-550 were reduced by about 40%, and a relatively slow, System 2-induced oxidation of cytochrome b₅₅₉ occurred which proceeded at a similar rate as the increase in yield of chlorophyll a fluorescence. The results indicate that at ?50°C two different photoreactions of System 2 occur. One consists of a photoreduction of the primary electron acceptor associated with C-550, accompanied by the oxidation of an unknown electron donor; the other is less efficient and results in the photooxidation of cytochrome b₅₅₉.     

Light-induced changes of fluorescence and absorbance in spinach chloroplasts at −40 °C

1. 1. Spinach chloroplasts were stored in the dark for at least 1 h, rapidly cooled to −40 °C, and illuminated with continuous light or short saturating flashes. In agreement with the measurements of Joliot and Joliot, chloroplasts that had been preilluminated with one or two flashes just before cooling showed a less efficient increase in the yield of chlorophyll a fluorescence upon illumination at −40 °C than dark-adapted chloroplasts. The effect disappeared below −150 °C, but reappeared again upon warming to −40 °C. Little effect was seen at room temperature in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU), added after the preillumination.

2. 2. Light-induced absorbance difference spectra at −40 °C in the region 500–560 nm indicated the participation of two components, the socalled 518-nm change (P518) and C-550. After preillumination with two flashes the absorbance change at 518 nm was smaller, and almost no C-550 was observed. After four flashes, the bands of C-550 were clearly visible again.

3. 3. The fluorescence increase and the absorbance change at 518 nm showed the same type of flash pattern with a minimum after the second and a maximum at the fourth flash. In the presence of 100 μM hydroxylamine, the fluorescence response was low after the fourth and high again after the sixth flash, which confirmed the hypothesis that the flash effect was related to the so-called S-state of the electron transport pathway from water to Photosystem 2.

4. 4. The kinetics of the light-induced absorbance changes were the same at each wavelength, and, apart from the size of the deflection, they were independent of preillumination. Flash experiments indicated that the absorbance changes were a one-quantum reaction. This was also true for the fluorescence increase in dark-adapted chloroplasts, but with preilluminated chloroplasts several flashes were needed to approximately saturate the fluorescence yield.

5. 5. The results are discussed in terms of a mechanism involving two electron donors and two electron acceptors for System 2 of photosynthesis.

Thermoluminescence study of charge recombination in Photosystem II at low temperatures. II. Oscillatory properties of the Zv and A thermoluminescence bands in chloroplasts dark-adapted for various time periods

The oscillations of the Z_V and A thermoluminescence bands were investigated in spinach chloroplasts which had been dark-adapted for various time periods and subjected to a series of flashes at +2°C before continuous illumination at various low temperatures. When excited with continuous light below −65°C, the Z_V band exhibited period-4 oscillation, with maxima on preflashes 0, 4 and 8. Above −65°C, the oscillation pattern depended greatly on the dark-adaptation period of the chloroplasts. In preilluminated samples (15 s light followed by 3 min dark), when the Q_B pool is half oxidized, the oscillation of the thermoluminescence intensity measured at −50°C was similar to that observed below −65°C. However, after the thorough dark-adaptation of the chloroplasts (6 h), when the major fraction of the Q_B pool is assumed to be oxidized, a binary oscillation appeared in the oscillation pattern, with maxima at odd flash numbers. Below −65°C, period-2 oscillation of the Z_V band could not be induced by the dark-adaptation of the chloroplasts, suggesting an inhibition of electron exchange between Q_A and Q_B. Upon excitation of the chloroplasts with continuous light at −30°C, the A band oscillated with a periodicity of 4 with maxima at preflash numbers 2 and 6. At pH 7.5, the period-4 oscillation was converted into a period-2 oscillation by thorough dark-adaptation of the chloroplasts (24 h). Model calculations of the oscillatory patterns suggest that the period-4 oscillations of the Z_V and A bands are determined by the concentrations [S₀] + [S₁] and [S₂] + [S₃], respectively, which are present after the preflashes prior to the low-temperature continuous illumination. The period-2 oscillations in the amplitudes of the Z_V and A bands reflect the changes occurring in the redox state of the Q_B pool in a sequence of flashes. The possible relationship between the characteristics of the Z_V and A bands and the temperature-dependence of the S state transitions was investigated. Comparison of the amplitudal changes of the B (S₂Q⁻_B and S₃Q⁻_B recombination) and Q (S₂Q⁻_A recombination) thermoluminescence bands as a function of the excitation temperature suggests that the S₂ → S₃ and S₃ → S₄ transitions are blocked at about −65 and −40°C, respectively. It is also concluded that the thermoluminescence intensity emitted by the reaction center is about twice as high in the S₃ state as in the S₂ state.     

Charge accumulation and recombination in Photosystem II studied by thermoluminescence. I. Participation of the primary acceptor Q and secondary acceptor B in the generation of thermoluminescence of chloroplasts

In the glow curves of chloroplasts excited by a series of flashes at +1°C the intensity of the main thermoluminescence band appearing at +30°C (B band; B, secondary acceptor of Photosystem II) exhibits a period-4 oscillation with maxima on the 2nd and 6th flashes indicating the participation of the S₃ state of the water-splitting system in the radiative charge recombination reaction. After long-term dark adaptation of chloroplasts (6 h), when the major part of the secondary acceptor pool (B pool) is oxidized, a period-2 contribution with maxima occurring at uneven flash numbers appears in the oscillation pattern. The B band can even be excited at ?160°C as well as by a single flash in which case the water-splitting system undergoes only one transition (S₁ → S₂). The experimental observations and computer simulation of the oscillatory patterns suggest that the B band originates from charge recombination of the S₂B^? and S₃B^? redox states. The half-time of charge recombination responsible for the B band is 48 s. When a major part of the plastoquinone pool is reduced due to prolonged excitation of the chloroplasts by continuous light, a second band (Q band; Q, primary acceptor of Photosystem II) appears in the glow curve at +10°C which overlaps with the B band. In chloroplasts excited by flashes prior to DCMU addition only the Q band can be observed showing maxima in the oscillation pattern at flash numbers 2, 6 and 10. The Q band can also be induced by flashes after DCMU addition which allows only one transition of the water-splitting system (S₁ → S₂). In the presence of DCMU, electrons accumulate on the primary acceptor Q, thus the Q band can be ascribed to the charge recombination of either the S₂Q^? or S₃Q^? states depending on whether the water-splitting system is in the S₂ or the S₃ state. The half-time of the back reaction of Q^? with the donor side of PS II (S₂ or S₃ states) is 3 s. It was also observed that in a sequence of flashes the peak positions of the Q and B bands do not depend on the advancement of the water-splitting system from the S₂ state to the S₃ state. This result implies that the midpoint potential of the water-splitting system remains unmodified during the S₂ → S₃ transition.     

A demonstration of energy transfer from photosystem II to photosystem I in chloroplasts

Photosystem I activity of Tris-washed chloroplasts was measured at room temperature as the rate of photoreduction of NADP and as the rate of oxygen uptake mediated by methyl viologen in both cases using dichlorophenolindophenol plus ascorbate as the source of electrons for Photosystem I. With both assay systems the rate of electron transport by Photosystem I was stimulated approx. 20 % by the addition of 3-(3,4-dichlorophenyl)-1, 1-dimethylurea which caused the Photosystem II reaction centers to close. Photosystem I activity of chloroplasts was measured at low temperature as the rate of photooxidation of P-700. Chloroplasts suspended in the presence of hydroxylamine and 3-(3,4-dichlorophenyl)-1, 1-dimethylurea were frozen to ?196 °C after adaptation to darkness or after a preillumination at room temperature. The Photosystem II reaction centers of the frozen dark-adapted sample were all open; those of the preilluminated sample were all closed. The rate of photooxidation of P-700 at ?196 °C with the preilluminated sample was approx. 25 % faster than with the dark-adapted sample. We conclude from both the room temperature and the low temperature experiments that there is greater energy transfer from Photosystem II to Photosystem I when the Photosystem II reaction centers are closed and that these results are a direct demonstration of spillover.     

The kinetics of light-induced changes of C-550, cytochrome b559 and fluorescence yield in chloroplasts at low temperature

The kinetics of the photoreduction of C-550, the photooxidation of cytochrome b₅₅₉ and the fluorescence yield changes during irradiation of chloroplasts at ?196 °C were measured and compared. The photoreduction of C-550 proceeded more rapidly than the photooxidation of cytochrome b₅₅₉ and the fluorescence yield increase followed the cytochrome b₅₅₉ oxidation. These results suggest that fluorescence yield under these conditions indicates the dark reduction of the primary electron donor to Photosystem II, P680⁺, by cytochrome b₅₅₉ rather than the photoreduction of the primary electron acceptor.The photoreduction of C-550 showed little if any temperature dependence over the range of ?196 to ?100 °C. The amount of cytochrome b₅₅₉ photooxidized was sensitive to temperature decreasing from the maximal change at temperatures between ?196 to ?160 °C to no change at ?100 °C. To the extent that the reaction occurred at temperatures between ?160 and ?100 °C the rate was largely independent of temperature. The rate of the fluorescence increase was dependent on temperature over this range being 3–4 times more rapid at ?100 than at ?160 °C. At ?100 °C the light-induced fluorescence increase and the photoreduction of C-550 show similar kinetics. The temperature dependence of the fluorescence induction curve is attributed to the temperature dependence of the dark reduction of P680⁺.The intensity dependence of the photoreduction of C-550 and of the photooxidation of cytochrome b₅₅₉ are linear at low intensities (below 200 μW/cm²) but fall off at higher intensities. The failure of reciprocity in the photoreduction of C-550 at the higher intensities is not explained by the simple model proposed for the Photosystem II reaction centers.     

Studies on the mechanism of ADRY agents (agents accelerating the deactivation reactions of water-splitting enzyme system Y) on thermoluminescence emission

The effect of 2-(3-chloro-4-trifluoromethyl)anilino-3,5-dinitrothiophene (ANT-2p), known to be the most powerful ADRY agent (Renger, G. (1972) Biochim. Biophys. Acta 256, 428–439), on thermoluminescence has been investigated. Two thermoluminescence bands were analyzed: (a) the emission peaking at about 20–30°C caused by warming up of untreated chloroplasts, illuminated with a single 5 μs flash at room temperature and frozen rapidly to 77 K; and (b) the band emitted in the range of ?10 up 10°C after warming of chloroplast suspensions containing 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) which were illuminated with a single 5 μs flash at ?15°C and frozen rapidly at 77 K. These bands were attributed to the recombination of the B ^?S₂(S₃) and X-320 ^?S₂ states, respectively (Rutherford, A.W., Crofts, A.R. and Inoue, Y. (1982) Biochim. Biophys. Acta 682, 457–465). It was found that: (1) The B ^?S₂(S₃) band is markedly diminished at very low ANT-2p concentrations of less than one molecule per 2000 chlorophylls. (2) The inhibition of the X-320 ^?S₂ band requires significantly higher concentrations of ANT-2p (50% peak reduction at one ANT-2p molecule per 100 chlorophylls). (3) Preflashing at room temperature before cooling to ?15°C diminishes the X-320 ^?S₂ band significantly in the presence of ANT-2p, while almost no effect is observed in its absence. (4) The state X-320 ^?S₂ decays monoexponentially with a half-lifetime of 2 min at ?15°C in the absence of ANT-2p. In the presence of one ANT-2p molecule per 800 chlorophylls the decay becomes biphasic with half-lifetimes of 0.5 and 2 min and an amplitude ratio of 2:3, respectively. The results obtained can be explained consistently by the function of ANT-2p as an ADRY agent acting as a mobile species within the thylakoid membrane at room temperature. At subzero temperatures, a ‘fixed-place’ mechanism appears to be operative. The implications for the ADRY effect and thermoluminescence are discussed.     

Correlation between the activity of membrane-bound ATPase and the decay rate of flash-induced 515-nm absorbance change in chloroplasts in intact leaves,assayed by means of rapid isolation of chloroplasts

(1) The relationship between activation of the membrane-bound ATPase and the stimulation of dissipation of the flash-induced membrane potential by preillumination was studied in intact spinach leaves by measuring the ATPase activity of rapidly isolated chloroplasts and the decay of the flash-induced 515-nm absorbance change (ΔA₅₁₅) in intact leaves. (2) The decay of ΔA₅₁₅ was accelerated by preillumination. The ΔA₅₁₅ decay in leaves treated with N,N′-dicyclohexylcarbodiimide (DCCD) became slower and was not accelerated by preillumination. However, treatment with DCCD did not lower the intensity of delayed fluorescence. (3) Membrane-bound ATPase of chloroplasts which were rapidly isolated from the preilluminated leaves (90 s preparation time) showed a higher activity (over 200 μmol P_i/mg chlorophyll per h in the case of 2-min preillumination) than that of chloroplasts isolated from dark-adapted leaves. (4) The acceleration of ΔA₅₁₅ decay and the activation of ATPase showed similar dependences on illumination time in intact leaves. 3-(3′,4′-Dichlorophenyl)-1,1-dimethylurea, carbonyl cyanide p-chlorophenylhydrazone and DCCD inhibited the activation of ATPase and the acceleration of the ΔA₅₁₅ decay by preillumination. (5) The ATPase activity of chloroplasts isolated from illuminated leaves showed a single exponential decay (‘dark inactivation in vitro’). The ATPase activity induced by illuminating the leaves became lower as the dark interval between illumination and the isolation of chloroplasts was increased (‘dark inactivation in vivo’). The time course of the decay of activity had a lag and showed a sigmoidal curve when plotted semilogarithmically. The decay had an apparent half-time of 25 min. (6) The recovery of the accelerated ΔA₅₁₅ decay in preilluminated leaves to the original slow rate showed a sigmoidal decay similar to that of the activity of ATPase in intact leaves with a half-time of about 23 min in the dark. (7) It was concluded that the decay rate of ΔA₅₁₅ reflected the chloroplast ATPase activity in intact leaves and that the ion conductance of thylakoid membrane was mainly determined by the H⁺ flux through the ATPase, the activity of which was increased after the formation of the high-energy state.     

Photoactivation of Electrogenic Activity in Chloroplasts and Its Relation to Photoinduced Swelling of Thylakoids

In patch-clamp experiments on isolated chloroplasts of Peperomia metallica Lind. et Rodig. (Piperaceae), the replacement of 50 mM KCl in a medium with 50 mM NH₄Cl strongly influenced the parameters of photocurrent known to reflect the generation of electric potential in thylakoids. The addition of NH⁺ ₄to the medium modified the induction curves of the photocurrent as well as the currents induced by single-turnover flashes in preilluminated chloroplasts. Under the action of a prolonged light pulse (1 s), the steady-state current was much higher in the ammonium-containing medium than in the presence of K⁺. Preillumination of a dark-adapted chloroplast with a 1-s light pulse suppressed the current induced by a single-turnover flash (6 s) in the presence of K⁺ but caused an elevation (by 50–150%) of the flash-induced current and shortening of its relaxation time in the presence of NH⁺ ₄. The origin of different induction kinetics for the photocurrent in K⁺ and NH⁺ ₄ media is partly clear, because ammonium prevents generation of the pH gradient and, subsequently, eliminates the pH-dependent suppression of the electron transport rate. However, this does not explain the origin of NH⁺ ₄-dependent photostimulation of the current generated by single-turnover flashes. This phenomenon arises from the thylakoid swelling caused by the accumulation of NH⁺ ₄ in the lumen and from the respective changes in the network resistances. The network element most sensitive to thylakoid swelling is the lateral resistance of the lumen: it decreases upon enlargement of the cross-section area. Stimulation of the flash-induced current by preillumination in the presence of NH⁺ ₄ was accompanied by accelerated relaxation of the current, indicating that the phenomena observed are caused by the reduction of network resistance involved in the discharge of the membrane capacity. Thus, the light-induced structural changes in the thylakoid system have a marked effect on the currents measured with the patch-clamp technique.     

Charge accumulation and recombination in Photosystem II studied by thermoluminescence. II. Oscillation of the C band induced by flash excitation

The characteristics of the thermoluminescence band appearing at +50°C in the glow curve (C band) was investigated in maize chloroplasts. The C band, which had a half-time of 10 min, could be charged in the presence of DCMU, and its amplitude significantly increased if preilluminated chloroplasts were reexcited after DCMU addition. Inactivation of the water-splitting system by hydroxylamine- or Tris-treatment did not abolish the C band. In chloroplasts subjected to various numbers of flashes before DCMU addition, the amplitude of the C band exhibited oscillation patterns which were markedly dependent upon dark adaptation of chloroplasts. Flash excitation of chloroplasts preilluminated by continuous light for 30 s prior to 5 min dark adaptation resulted in a period-4 oscillation with maxima occurring at flash numbers 0, 4, 8, 12. After a 6-h dark-adaptation of chloroplasts the period-4 oscillation was superimposed with a period-2 oscillation. The oscillatory patterns were simulated by model calculations and the possible origin of the C band is discussed.     

Effects of chloride depletion on electron donation from the water-oxidizing complex to the photosystem II reaction center as measured by the microsecond rise of chlorophyll fluorescence in isolated pea chloroplasts

The role of Cl^? in the electron transfer reactions of the oxidizing side of Photosystem II (PS II) has been studied by measuring the fluorescence yield changes corresponding to the reduction of P⁺-680, the PS II reaction center chlorophyll, by the secondary PS II donor, Z. In Cl^?-depleted chloroplasts, a rapid rise in fluorescence yield was observed following the first and second flashes, but not during the third or subsequent flashes. These results indicate that there exists an additional endogenous electron donor beyond P-680 and Z in Cl^?-depleted systems. In contrast, the terminal endogenous donor on the oxidizing side of PS II in Tris-washed preparations has previously been shown to be Z, the component giving rise to EPR signals II_f and II_vf. The rate of reduction of P⁺-680 in the Cl^?-depleted chloroplasts was as rapid as that measured in uninhibited systems, within the time resolution of our instrument. Again, this is in contrast to Tris-washed preparations in which a dramatic decrease in the rate if this reaction has been previously reported. We have also carried out a preliminary study on the rate of rereduction of Z⁺ in the Cl^?-depleted system. Under steady-state conditions, the reduction half-time of Z⁺ in uninhibited systems was about 450 μs, while in the Cl^?-depleted chloroplasts, the reduction of Z⁺ was biphasic, one phase with a half-time of about 120 ms, and a slower phase with a half-time of several seconds. The appearance of the quenching state due to P⁺-680 observed following the third flash on excitation of Cl^?-depleted chloroplasts was delayed by two flashed when low concentrations of NH₂OH (20–50 μM) were included in the medium. Hydrazine at somewhat higher concentrations showed the same effect. This is taken to indicate that the reactions leading to PS II oxidation of NH₂OH or NH₂NH₂ are uninhibited by Cl^? depletion. Addition of NH₂OH at low concentrations to Tris-washed chloroplasts did not alter the pattern of the fluorescence yield, indicating that the reactions leading to the NH₂OH oxidation present in Cl^?-depleted systems are absent following Tris inhibition. The results are discussed in terms of an inhibition by Cl^? depletion of the reactions of the oxygen-evolving complex. It is suggested that no intermediary redox couple exists between the oxygen-evolving complex and Z, and that Z⁺ is reduced directly by Mn of the complex. In terms of the S-state model, Cl^? depletion appears to inhibit the advancement of the mechanism beyond S₂, but not to inhibit the transitions from S₀ to S₁, or from S₁ to S₂.     

Oxygen-evolution patterns from spinach Photosystem II preparations

Patterns of O₂ evolution resulting from sequences of short flashes are reported for Photosystem (PS) II preparations isolated from spinach and containing an active, O₂-evolving system. The results can be interpreted in terms of the S-state model developed to explain the process of photosynthetic water splitting in chloroplasts and algae. The PS II samples display damped, oscillating patterns of O₂ evolution with a period of four flashes. Unlike chloroplasts, the flash yields of the preparations decay with increasing flash number due to the limited plastoquinone acceptor pool on the reducing side of PS II. The optimal pH for O₂ evolution in this system (pH 5.5–6.5) is more acidic than in chloroplasts (pH 6.5–8.0). The O₂-evolution, inactivation half-time of dark-adapted preparations was 91 min (on the rate electrode) at room temperature. Dark-inactivation half-times of 14 h were observed if the samples were aged off the electrode at room temperature. Under our conditions (experimental conditions can influence flash-sequence results), deactivation of S₃ was first order with a half-time of 105 s while that of S₂ was biphasic. The half-times for the first-order rapid phase were 17 s (one preflash) and 23 s (two preflashes). The longer S₂ phase deactivated very slowly (the minimum half-time observed was 265 s). These results indicate that deactivation from S₃ → S₂ → S₁, thought to be the dominant pathway in chloroplasts, is not the case for PS II preparations. Finally, it was demonstrated that the ratio of S₁ to S₀ can be set by previously developed techniques, that S₀ is formed mostly from activated S₃ (S₄), and that both S₀ and S₁ are stable in the dark.     

A diffusional analysis of the temperature sensitivity of the Mg2+-induced rise of chlorophyll fluorescence from pea thylakoid membranes

The kinetics of the chlorophyll fluorescence rise induced by adding 20 mM MgCl₂ to a suspension of isolated pea chloroplasts treated with 3-(3,4-dichlorophenyl)-1, 1-dimethylurea (DCMU) have been examined experimentally and theoretically as a function of temperature. The application of similarity arguments and particle aggregation theory to the experimental results suggests that at the first approximation, the salt-induced time-dependent fluorescence changes may be described by the diffusion-controlled lateral movement of Photosystem II pigment-protein complexes. From an analysis of the temperature dependence of the fluorescence changes, estimates obtained for the lateral diffusion coefficients were 1.85 · 10^?12–3.08 · 10^?11 cm²/s over the temperature range 10°C ? T?30°C.     

Effect of temperature on senescing detached rice leaves: I. Photoelectron transport activity of chloroplasts

Detached rice(Oryza sativaL cv Mousouri)leaves were induced to senesce in darkness at 0°C(cold), 27°C(room temperature) and 40°C(heat). 2,6-dichlorophenol indophenol (DCPIP) Hill reaction activity of chloroplasts isolated from senescing leaves under all experimental temperatures with H₂O, Mn²⁺ or diphenyl carbazide (DPC) as electron donor declined during the period of incubation. Since DPC and Mn²⁺ augmented 2,6-dichlorophenol indophenol photoreduction by chloroplasts from senescing leaves, damage and/or change in the conformation of a site between H₂O and DCPIP in photosystem II (PS II) is suggested. Heat caused a faster decline of the Hill activity compared to cold or room temperature. However, cold treatment showed no significant effect on the photoelectron transport from H₂O to DCPIP compared with room temperature.     

Laser-flash-activated electron paramagnetic resonance studies of primary photochemical reactions in chloroplasts

Electron paramagnetic resonance studies of the primary reactants of Photosystems I and II have been conducted at cryogenic temperatures after laser-flash activation with monochromatic light.P-700 photooxidation occurs irreversibly in chloroplasts and in Photosystem I fragments after activation with a 730 nm laser flash at a temperature of 35 °;K. Flash activation of chloroplasts or Photosystem II chloroplast fragments with 660 nm light results in the production of a free-radical signal (g = 2.002, linewidth ～ 8 gauss) which decays with a half-time of 5.0 ms at 35 °;K. The half-time of decay is independent of temperature in the range of 10–77 °;K. This reversible signal can be eliminated by preillumination of the sample at 35 °;K with 660 nm light (but not by 730 nm light), by preillumination with 660 nm light at room temperature in the presence of 3-(3′, 4′-dichlorophenyl)-1,1′-dimethylurea (DCMU) plus hydroxylamine, or by adjustment of the oxidation-reduction potential of the chloroplasts to — 150 mV prior to freezing. In the presence of ferricyanide (20–50 mM), two free-radical signals are photoinduced during a 660 nm flash at 35 °;K. One signal decays with a half-time of 5 ms, whereas the second signal is formed irreversibly. These results are discussed in terms of a current model for the Photosystem II primary reaction at low temperature which postulates a back-reaction between P-680⁺ and the primary electron acceptor.     

Oscillation of delayed luminescence from PS II: recombination of S2Q−B and S3Q−B

Luminescence decaying in the seconds to minutes time scale was studied in spinach chloroplasts and the following results were obtained: (1) After a series of flashes a slow phase which decays in the tens of seconds to minutes time scale was observed to oscillate with a pattern characteristic of S₂Q^?_B and S₃Q^?_B recombination. This phase was lost upon Tris-treatment or upon the addition of DCMU. (2) After every flash a small faster phase of luminescence decaying in the seconds time scale was also present. This phase progressively increased with increasing numbers of flashes but when methyl viologen was present no such progressive increase of this phase occurred. In the presence of DCMU this seconds time scale luminescence was greatly increased. This phase of luminescence is attributed to S₂Q^?_A recombination. (3) Tris-treatment resulted in the appearance of an even faster phase of luminescence which may be due to Z⁺Q^?_B recombination. These results demonstrate a close correlation of the kinetics of luminescence decay with thermoluminescence emission temperature.     

Photooxidation of cytochrome b559 and the electron donors in chloroplast Photosystem II

The effect of light on the reaction center of Photosystem II was studied by differential absorption spectroscopy in spinach chloroplasts.

At − 196 °C, continuous illumination results in a parallel reduction of C-550 and oxidation of cytochrome b₅₅₉ high potential. With flash excitation, C-550 is reduced, but only a small fraction of cytochrome b₅₅₉ is oxidized. The specific effect of flash illumination is suppressed if the chloroplasts are preilluminated by one flash at 0 °C.

At − 50 °C, continuous illumination results in the reduction of C-550 but little oxidation of cytochrome b₅₅₉. However, complete oxidation is obtained if the chloroplasts have been preilluminated by one flash at 0 °C. The effect of preillumination is not observed in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea.

A model is discussed for the reaction center, with two electron donors, cytochrome b₅₅₉ and Z, acting in competition. Their respective efficiency is dependent on temperature and on their states of oxidation. The specific effect of flash excitation is attributed to a two-photon reaction, possibly based on energy-trapping properties of the oxidized trap chlorophyll.