Chlorophyll-protein complexes of a Codium species,including a light-harvesting siphonaxanthin-Chlorophylla ab-protein complex,an evolutionary relic of some Chlorophyta

Eight chlorophyll-protein complexes were isolated from thylakoid membranes of a Codium species, a marine green alga, by mild SDS-polyacrylamide gel electrophoresis. CP 1a¹, CP 1a², CP 1a³ and CP 1a⁴ were partially dissociated Photosystem (PS) I complexes, which in addition to the core reaction centre complex, CP 1, possessed PS I light-harvesting complexes containing chlorophyll (Chl) a, Chl b and siphonaxanthin. LHCP¹ and LHCP³ are orange-brown green chlorophyll $\text{a}\text{b-}\text{proteins}$ ($\text{Chl}\text{a}\text{Chl}\text{b}$ ratios of 0.66) that contain siphonaxanthin and its esterified form, siphonein. CP a and CP 1, the core reaction centre complexes of PS II and PS I, respectively, had similar spectral properties to those isolated from other algae or higher plants. These P-680- or P-700-Chl a-proteins are universally distributed among algae and terrestrial plants; they appear to be highly conserved and have undergone little evolutionary adaptation. Siphonaxanthin and siphonein which are present in the Codium light-harvesting complexes of PS II and PS I are responsible for enhanced absorption in the green region (518 and 538 nm). Efficient energy transfer from both xanthophylls and Chl b to only Chl a in Codium light-harvesting complexes, which have identical fluorescence emission spectra at 77 K to those of the lutein-Chl $\text{a}\text{b-}\text{proteins}$ ($\text{Chl}\text{a}\text{Chl}\text{b}$ ratios of 1.2) of most green algae and all higher plants, proved that the molecular arrangement of these light-harvesting pigments was maintained in the isolated Codium complexes. The siphonaxanthin-Chl $\text{a}\text{b-}\text{proteins}$ allow enhanced absorption of blue-green and green light, the predominant light available in deep ocean waters or shaded subtidal marine habitats. Since there is a variable distribution of lutein, siphonaxanthin and siphonein in marine green algae and siphonaxanthin is found in very ancient algae, these novel siphonein-siphonaxanthin-Chl $\text{a}\text{b-}\text{proteins}$ may be ancient light-harvesting complexes which were evolved in deep water algae.     

Possible effects of the detachment of stromal lamellae from granal stacks on salt-induced changes in spillover. A study by sonication of chloroplasts

Salt-induced chlorophyll fluorescence and spillover changes in control and briefly sonicated chloroplasts have been studied under conditions where Photosystem II traps are closed. In a low-salt medium containing 10 mM KCl, control envelope-free chloroplasts exhibited good spillover, as measured by low chlorophyll fluorescence yield at room temperature, a high ratio of the fluorescence peaks $\text{F}{}_{735}\text{F}{}_{685}$ at 77 K, and increased Photosystem I activity in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea and Photosystem II light. In contrast, when stacked chloroplasts were briefly sonicated and subsequently diluted into a low-salt medium, a high fluorescence yield at room temperature and a low ratio of $\text{F}{}_{735}\text{F}{}_{685}$ at 77 K persisted. When unstacked chloroplasts were sonicated and then diluted into a high-salt medium, the room temperature fluorescence yield remained low. The results are interpreted in terms of a model relating the changes in chlorophyll fluoresecence with the lateral diffusion of Photosystem I and Photosystem II chlorophyll-protein complexes in the plane of the thylakoid membrane creating randomized or segregated domains, depending on the degree of electrostatic screening of surface charges (Barber, J. (1980) FEBS Lett. 188, 1–10). It is argued that brief sonication of stacked chloroplasts separates stromal membranes from granal stacks, thus limiting the inter-mixing of the photosystems via lateral diffusion even when the ionic composition of the medium is varied. Consequently energy transfer from Photosystem II to Photosystem I is relatively poor and chlorophyll fluorescence from Photosystem II is enhanced. The loss of the salt effect on sonicated unstacked membranes can also be accommodated by the model. In this case it seems that the generation of small membrane fragments does not allow the normal salt-induced phase separation of the pigment-protein complexes to occur.     

Antenna function of a chlorophyll ab protein complex of Photosystem I

The functional role of a chlorophyll $\text{a}\text{b}$ complex associated with Photosystem I (PS I) has been studied. The rate constant for P-700 photooxidation, K_P-700, which under light-limiting conditions is directly proportional to the size of the functional light-harvesting antenna, has been measured in two PS I preparations, one of which contains the chlorophyll $\text{a}\text{b}$ complex and the other lacking the complex. K_P-700 for the former preparation is half of that of the preparation which has the chlorophyll $\text{a}\text{b}$ complex present. This difference reflects a decrease in the functional light-harvesting antenna in the PS I complex devoid of the chlorophyll $\text{a}\text{b}$ complex. Experiments involving reconstitution of the chlorophyll $\text{a}\text{b}$ complex with the antenna-depleted PS I preparation indicate a substantial recovery of the K_P-700 rate. These results demonstrate that the chlorophyll $\text{a}\text{b}$ complex functions as a light-harvesting antenna in PS I.     

Effect of light quality on the composition and function of thylakoid membranes in atriplex triangularis

Light quality was shown to exert well-coordinated regulatory effects on the composition and function of the thylakoid membranes as well as on the photosynthetic rates of intact leaves from Atriplex triangularis grown in continuous blue, white and red lights (50 μE · m^?2 · s^?1). The higher photosynthetic rates in plants grown in blue light, as compared to those in white and red lights, resulted from marked changes in both light-harvesting complexes and electron carriers. The concentrations of electron carriers such as atrazine binding sites, plastoquinone, cytochromes b and f and P-700 on a chlorophyll basis were markedly increased in Atriplex grown in blue light; and the apparent light-harvesting antenna unit sizes of Photosystems I and II were greatly reduced. Consequently, the electron transport capacities of Photosystems I and II were also increased as was the coupling factor CF₁ activity. Atriplex grown in red light had lower photosynthetic rates than those grown in blue or white light by incorporating changes in the composition and function of the thylakoids in a direction opposite to those caused by growth in blue light. When these regulatory effects of light quality were compared with those of light quantity [6,7], it is clear that $\text{Chl}\text{a}\text{Chl}\text{b}$ ratios, electron transport capacities of Photosystems I and II, concentrations of plastoquinone, atrazine binding sites, coupling factor CF₁ activity and the apparent antenna unit size of Photosystem II are more affected by light quantity, whereas light quality has a greater influence on the concentration of P-700, the apparent antenna unit size of Photosystem I and the overall photosynthetic rates of intact leaves.     

Effects of cations upon chloroplast membrane subunit interactions and excitation energy distribution

When isolated chloroplasts from mature pea (Pisum sativum) leaves were treated with digitonin under “low salt” conditions, the membranes were extensively solubilized into small subunits (as evidenced by analysis with small pore ultrafilters). From this solubilized preparation, a photochemically inactive chlorophyll · protein complex (chlorophyll $\text{a}\text{b}$ ratio, 1.3) was isolated. We suggest that the detergent-derived membrane fragment from mature membranes is a structural complex within the membrane which contains the light-harvesting chlorophyll $\text{a}\text{b}$ protein and which acts as a light-harvesting antenna primarily for Photosystem II.Cations dramatically alter the structural interaction of the light-harvesting complex with the photochemically active system II complex. This interaction has been measured by determining the amount of protein-bound chlorophyll b and Photosystem II activity which can be released into dispersed subunits by digitonin treatment of chloroplast lamellae. When cations are present to cause interaction between the Photosystem II complex and the light-harvesting pigment · protein, the combined complexes pellet as a “heavy” membranous fraction during differential centrifugation of detergent treated lamellae. In the absence of cations, the two complexes dissociate and can be isolated in a “light” submembrane preparation from which the light-harvesting complex can be purified by sucrose gradient centrifugation.Cation effects on excitation energy distribution between Photosystems I and II have been monitored by following Photosystem II fluorescence changes under chloroplast incubation conditions identical to those used for detergent treatment (with the exception of chlorophyll concentration differences and omission of detergents). The cation dependency of the pigment · protein complex and Photosystem II reaction center interactions measured by detergent fractionation, and regulation of excitation energy distribution as measured by fluorescence changes, were identical. We conclude that changes in substructural organization of intact membranes, involving cation induced changes in the interaction of intramembranous subunits, are the primary factors regulating the distribution of excitation energy between Photosystems II and I.     

Covalent modification of chloroplast Photosystem II polypeptides by p-nitrothiophenol

Illumination of the chlorophyll $\text{a}\text{b}$ light-harvesting complex in the presence of $\text{p-}\text{nitrothio}\text{[}{}^{14}\text{C]phenol}$ caused quenching of fluorescence emission at 685 nm (77 K) relative to 695 nm and covalent modification of light-harvesting complex polypeptides. Fluorescence quenching saturated with one p-nitrothiophenol bound per light-harvesting complex polypeptide (10–13 chlorophylls); $\text{1}\text{2}$ maximal quenching occurred with one p-nitrothiophenol bound per light-harvesting complex polypeptides (190–247 chlorophylls). This result provides direct evidence for excitation energy transfer between light-harvesting complex subunits which contain 4–6 polypeptides plus 40–78 chlorophylls per complex.Illumination of chloroplasts or Photosystem II (PS II) particles in the presence of $\text{p-}\text{nitrothio}\text{[}{}^{14}\text{C]phenol}$ caused inhibition of PS II activity and labeling of several polypeptides including those of 42–48 kilodaltons previously identified as PS II reaction center polypeptides. In chloroplasts, inhibition of oxygen evolution accelerated p-nitrothiophenol modification reactions; DCMU or donors to PS II decreased p-nitrothiophenol modification. These results are consistent with the hypothesis that accumulation of oxidizing equivalents on the donor side of PS II creates a ‘reactive state’ in which polypeptides of PS II are susceptible to p-nitrothiophenol modification.     

Changes in the redox state of the secondary acceptor of Photosystem II associated with light-induced thylakoid protein phosphorylation

Thylakoid membrane protein phosphorylation affects photochemical reactions of Photosystem II. Incubation of thylakoids in the light with ATP leads to: (1) an increase in the amplitude of three components (4–6, 25–45 and 280–300 μs) of delayed light emission after a single flash without any change in their kinetics; (2) a reduction of the flash-dependent binary oscillations of chlorophyll a fluorescence yield associated with electron transfer from the primary quinone acceptor, Q, to the secondary quinone acceptor, B; (3) an increase in the $\text{B}{}^{\mathrm{?}}\text{B}$ ratio resulting from an increase in stability of the semiquinone anion during dark adaptation; and (4) no change in the redox state of the plastoquinone pool as determined by flash-induced photooxidation of the Photosystem I reaction center, P-700. All the above observations are reversible upon dephosphorylation of the thylakoid membranes. These data are explained by a protein phosphorylation-induced stabilization of the bound semiquinone anion, B^?. It is proposed that this increased stability may be due to an alteration in the accessibility of an endogenous reductant to B, or to an increase in dissipative cycling of charge around Photosystem II.     

Thylakoid protein phosphorylation during State 1—State 2 transitions in osmotically shocked pea chloroplasts

In osmotically shocked pea chloroplasts illuminated with modulated blue-green light (light 2), phosphorylation of the light-harvesting chlorophyll $\text{a}\text{b-}\text{protein}$ complex (LHCP) accompanies the slow decrease in modulated fluorescence that indicates adaptation to light absorbed predominantly by Photosystem II (State 2). On subsequent additional illumination with continuous far-red light (absorbed predominantly by Photosystem I; light 1) both effects are reversed: modulated chlorophyll fluorescence emission increases (indicating adaptation towards State 1) and LHCP is dephosphorylated. Net phosphorylation and dephosphorylation of LHCP induced by light 2 and excess light 1, respectively, occur on the same time scale as the ATP-dependent chlorophyll fluorescence changes indicative of State 2 and State 1 transitions. The phosphatase inhibitor NaF (10 mM), stimulates the effect of blue-green light on fluorescence and prevents the effect of far-red light. These results provide a demonstration that light of different wavelengths can control excitation energy distribution between the two photosystems via the plastoquinol-activated LHCP phosphorylation mechanism suggested previously (Allen, J.F., Bennett, J., Steinback, K.E. and Arntzen, C.J. (1981) Nature 291, 25–29; and Horton, P. and Black, M.T. (1980) FEBS Lett. 119, 141–144).     

State 1-state 2 transition in leaves and its association with ATP-induced chlorophyll fluorescence quenching

By using chlorophyll fluorescence, a study has been made of changes in spillover of excitation energy from Photosystem (PS) II to PS I associated with the State 1–State 2 transition in intact pea and barley leaves and in isolated envelope-free chloroplasts treated with ATP. (1) In pea leaves, illumination with light preferentially absorbed by PS II (Light 2) led to a condition of maximum spillover (state 2) while light preferentially absorbed by PS I induced minimum spillover condition (State 1) as judged from the redox state of Q and low-temperature emission spectra. The State 1–State 2 transitions took several minutes to occur, with the time increasing when the temperature was lowered from 19 to 6°C. (2) In contrast to the wild type, leaves of a chlorophyll b-less mutant barley did not exhibit a State 1–State 2 transition, suggesting the involvement of the light-harvesting chlorophyll $\text{a}\text{b-}\text{protein}$ complex in spillover changes in higher plants. (3) Spillover in isolated pea chloroplasts was increased by treatment with ATP either (a) in Light 2 in the absence of an electron acceptor or (b) in the dark in the presence of NADPH and ferredoxin. These observations can be interpreted in terms of the model that a more reduced state of plastoquinone activates the protein kinase which catalyzes phosphorylation of the light-harvesting chlorophyll $\text{a}\text{b-}\text{protein}$ complex (Allen, J.F., Bennett, J., Steinback, K.E. and Arntzen, C.J. (1981). Nature 291, 25–29). This process was found to be very temperature sensitive. (4) Pea chloroplasts illuminated in the presence of ATP seemed to exhibit a slight decrease in the degree of thylakoid stacking, and an increased intermixing of the two photosystems. (5) The possible mechanism by which protein phosphorylation regulates the State 1–State 2 changes in intact leaves is presented in terms of changes in the spatial relationship of two photosystems resulting from alteration in membrane organization.     

The influence of metabolic state on the level of phosphorylation of the light-harvesting chlorophyll-protein complex in chloroplasts isolated from maize mesophyll

The activity of the protein kinase that phosphorylates the light-harvesting chlorophyll-protein of Photosystem II (LHCP) has been investigated in intact chloroplasts isolated from maize mesophyll cells. Measurements of ³²P incorporation into LHCP, ATP concentration, $\text{ATP}\text{ADP}$ ratio, ΔpH, chlorophyll fluorescence and oxygen evolution were made in the presence of different metabolic substrates. Without added substrate a high level of LHCP phosphorylation was observed which was suppressed by addition of oxaloacetate or phosphoglycerate but stimulated by pyruvate. Whereas no correlation was observed between LHCP phosphorylation and adenylate status, a clear effect of redox state on protein kinase activity was observed. A correlation between a highly reduced electron-transfer chain (produced under conditions which favour cyclic electron flow) and the maximum level of protein phosphorylation was observed. The regulation of kinase activity and its dependence on electron transfer and carbon assimilation are discussed.     

Analysis of chlorophyll fluorescence induction curves in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea as a function of magnesium concentration and NADPH-activated light-harvesting chlorophyll ab-protein phosphorylation

The effect of Mg²⁺ concentration and phosphorylation of light-harvesting chlorophyll $\text{a}\text{b-}\text{protein}$ on various chlorophyll fluorescence induction parameters of isolated pea thylakoids has been studied. (1) Lowering the Mg²⁺ concentration from 3 to 0.4 mM decreases only the variable fluorescence (F_v) and the area above the induction curve while at the same time increasing the slow exponential component of the rise (β_max). (2) A further decrease in Mg²⁺ concentration from 0.4 to 0 mM decreases the initial (F₀) fluorescence level such that the ratio $\text{F}{}_{\mathrm{<mtext>v</mtext>}}\text{F}{}_{\mathrm{<mtext>m</mtext>}}$ increases slightly as does the area above the induction curve and β_max. (3) Thylakoid membranes, phosphorylated at 5 mM Mg²⁺, show an equal decrease in F_v and F₀, no change in the area above the induction curve and an increase in β_max. At 2 mM Mg²⁺, however, phosphorylation induced a more extensive quenching of F_v so that the $\text{F}{}_{\mathrm{<mtext>v</mtext>}}\text{F}{}_{\mathrm{<mtext>m</mtext>}}$ ratio was lowered and the area above the induction curve decreased while β_max increased. (4) When phosphorylated membranes were subsequently suspended in an Mg²⁺-free medium the effect on F₀ due to phosphorylation was found to be additive to that due to the absence of Mg²⁺. The effect of membrane phosphorylation on fluorescence is discussed in relation to the control of excitation energy distribution and shows that different mechanisms operate depending on the background Mg²⁺ levels. At high Mg²⁺ the phosphorylation seems to affect the absorption cross-section of Photosystem II while at lower Mg²⁺ levels there is an additional effect of increased spillover from Photosystem II to I.     

Preparation of O2-evolving Photosystem-II subchloroplasts from spinach

An O₂-evolving Photosystem II subchloroplast preparation was obtained from spinach chloroplasts, using low concentrations of digitonin and Triton X-100. The preparation showed an O₂ evolution activity equivalent to 20% of the uncoupled rate of fresh broken chloroplasts, but had no significant Photosystem-I-dependent O₂ uptake activity. The preparation showed a chlorophyll $\text{a}\text{b}$ ratio of 1.9 and a $\text{P-700}\text{chlorophyll}$ ratio of $\text{1}\text{2400}$. Absorption spectra at room temperature and fluorescence emission spectra of chlorophyll at 77 K suggested a significant decrease in Photosystem I antenna chlorophylls in the O₂-evolving Photosystem II preparation.     

Characterization of chlorophyll fluorescence quenching in chloroplasts by fluorescence spectroscopy at 77 K II. ATP-dependent quenching

In intact, uncoupled type B chloroplasts from spinach, added ATP causes a slow light-induced decline ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{≈ 3}\text{min}$) of chlorophyll a fluorescence at room temperature. Fluorescence spectra were recorded after fast cooling to 77 K and normalized with fluorescein as an internal standard. Related to the fluorescence quenching at room temperature, an increase in Photosystem (PS) I fluorescence (F₇₃₅) and a decrease in PS II fluorescence (F₆₉₅) were observed in the low-temperature spectra. The change in the $\text{F}{}_{735}\text{F}{}_{695}$ ratio was abolished by the presence of methyl viologen. Fluorescence induction at 77 K of chloroplasts frozen in the quenched state showed lowered variable (F_v) and initial (F₀) fluorescence at 690 nm and an increase in F₀ at 735 nm. The results are interpreted as indicating an ATP-dependent change of the initial distribution of excitation energy in favor of PS I, which is controlled by the redox state of the electron-transport chain and, according to current theories, is caused by phosphorylation of the light-harvesting complex.     

The chlorophyll-protein complexes of Acetabularia. A novel chlorophyll ab complex which forms oligomers

(1) Five minor chlorophyll-protein complexes were isolated from thylakoid membranes of the green alga Acetabularia by SDS-polyacrylamide gel electrophoresis, after SDS or octylglucoside solubilization. None of them were related to CP I (Photosystem I reaction center core) or CP II (chlorophyll $\text{a}\text{b}$ light-harvesting complex). (2) Two complexes (CPa-1 and CPa-2) contained only chlorophyll (Chl) a, with absorption maxima of 673 and 671 nm, and fluorescence emission maxima of 683 nm compared to 676 nm for CP II. The complexes had apparent molecular masses of 43–47 and 38–40 kDa, and contained a single polypeptide of 41 and 37 kDa, respectively. They each account for about 3% of the total chlorophyll. (3) Three complexes had identical spectra, with Chl $\text{a}\text{b}$ ratios of 3–4 compared to 2 for thylakoid membranes, and a pronounced shoulder around 485 nm indicating enrichment in carotenoids. One of them was the complex ‘CP 29’ (Camm, E.L. and Green, B.R. (1980) Plant Physiol. 66, 428–432) and the other two were slightly different oligomeric forms of CP 29. They could be formed from CP 29 during reelectrophoresis; but about half the complex was isolated originally in an oligomeric form. Together they account for at least 7% of the total chlorophyll. Their function is unknown.     

Orientation and linear dichroism of chloroplasts and sub-chloroplast fragments oriented in an electric field

Whole or broken spinach chloroplasts, bacterial chromatosphores and CPI chlorophyll · protein complexes in aqueous suspensions at room temperature can be oriented in externally applied electric fields. The orientation is observed by monitoring the electric field induced linear dichroism (LD). With whole chloroplasts a detectable LD signal is observed using voltages as low as 2–3 V (50 Hz alternating voltage) across an 0.3 cm electrode gap, and nearly complete orientation is observed at fields of 30 V · cm^?1. The wavelength dependence of the LD signals using either orienting electric fields ($\text{E}$) alone, or magnetic fields ($\text{B}$) alone, are similar but opposite in sign with $\text{E}$ and $\text{B}$ pointing in the same direction. The chloroplasts tend to orient in such a way that the membrane planes are parallel to $\text{E}$. The CPI complexes and bacterial chromatophores require much higher electric fields for orientation than whole chloroplasts (for CPI complexes E > 2000 V · cm^?1); rectangular, millisecond duration, voltage pulses are utilized for the observation of electric field induced LD spectra in these cases. Oriented CPI complexes exhibit LD maxima of the same sign at 685 and at 440 nm. The oriented chromatophores exhibit an LD spectrum of either positive or negative sign, depending on the wavelength. The mechanisms of the orientation are discussed.     

Picosecond time-resolved study of MgCl2-induced chlorophyll fluorescence yield changes from chloroplasts

The MgCl₂-induced chlorophyll fluorescence yield changes in broken chloroplasts, suspended in a cation-free medium, treated with 3,-(3′,4′-dichlorophenyl)-1,1-dimethylurea and pre-illuminated, has been investigated on a picosecond time scale. Chloroplasts in the low fluorescing state showed a fluorescence decay law of the form exp $\text{?At}{}^{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$, where A was found to be 0.052 $\text{ps}{}^{\mathrm{<mtext>?1</mtext><mtext>2</mtext>}}$, and may be attributed to the rate of spillover from Photosystem II to Photosystem I. Addition of 10 mM MgCl₂ produced a 50% increase in the steady-state fluorescence quantum yield and caused a marked decrease in the decay rate. The fluorescence decay law was found to be predominantly exponential with a 1/e lifetime of 1.6 ns. These results support the hypothesis that cation-induced changes in the fluorescence yield of chlorophyll are related to the variations in the rate of energy transfer from Photosystem II to Photosystem I, rather than to changes in the partitioning of absorbed quanta between the two systems.     

Zero field resonance and spin alignment of the triplet state of chloroplasts at 2°K

Microwave induced transitions in zero magnetic field have been observed in the photoinduced triplet of chloroplasts treated with dithionite by monitoring changes in the intensity of the 735 nm fluorescence band at 2°K. Similar results were obtained with chloroplasts treated with hydroxylamine plus 3-(3,4-dichlorophenyl)-1,1-dimethylurea and preillumination. The zero field parameters are $\text{D = 0.02794 ± 0.00007}\text{cm}{}^{\mathrm{?1}}$, $\text{E = 0.00382 ± 0.00007}\text{cm}{}^{\mathrm{?1}}$, i.e. equal to those of monomeric chlorophyll $\text{a}$ to within the experimental error. The photoinduced triplet appears to be linked to Photosystem II. This indicates that the low temperature 735 nm fluorescence band of chloroplasts is at least partly due to Photosystem II.     

The cation-dependence of the degree of protein phosphorylation-induced unstacking of pea thylakoids

Experiments are presented to show that the phosphorylation of the light-harvesting chlorophyll $\text{a}\text{b}\text{-}\text{protein}$ complex (LHC) induces structural reorganisation within the thylakoid membrane in response to the introduction of additional negative surface charges. The effect of cations of different valency on chlorophyll fluorescence measurements indicates that LHC-phosphorylation-induced reorganisation involves a change in the electrostatic screening capability of the added cation. At intermediate levels of cations (e.g., 1 or 2 mM Mg²⁺), which substantially stack non-phosphorylated membranes, it was found that membrane phosphorylation caused considerable unstacking as monitored by light scattering and electron microscopy. Concomitant with this was a large decrease in chlorophyll fluorescence indicative of randomisation of chlorophyll protein complexes which would result in an increase in energy transfer between the photosystems as well as an absorption cross-section change. At higher concentrations (e.g., above 5 mM Mg²⁺) a persistent ATP-induced decrease in chlorophyll fluorescence has been attributed to the displacement of charged phosphorylated LHC from the appressed granal to the non-appressed stromal lamellae, thus decreasing the absorption cross-section of Photosystem II. Under these circumstances only a small degree of unstacking was detected by light scattering and measurements of the percentage of thylakoid length which is stacked to form grana. However, when considered on a surface area basis, the structural changes observed can qualitatively account for the magnitude of the chlorophyll fluorescence quenching due to the lateral diffusion of LHC.     

Excitation spectra of chlorophyll fluorescence in spinach and barley chloroplasts at 4 K

Excitation spectra of chlorophyll a fluorescence in chloroplasts from spinach and barley were measured at 4.2 K. The spectra showed about the same resolution as the corresponding absorption spectra. Excitation spectra for long-wave chlorophyll a emission (738 or 733 nm) indicate that the main absorption maximum of the photosystem (PS) I complex is at 680 nm, with minor bands at longer wavelengths. From the corresponding excitation spectra it was concluded that the emission bands at 686 and 695 nm both originate from the PS II complex. The main absorption bands of this complex were at 676 and 684 nm. The PS I and PS II excitation spectra both showed a contribution by the light-harvesting chlorophyll $\text{a}\text{b}$ protein(s), but direct energy transfer from PS II to PS I was not observed at 4 K. Omission of Mg²⁺ from the suspension favored energy transfer from the light-harvesting protein to PS I. Excitation spectra of a chlorophyll b-less mutant of barley showed an average efficiency of 50–60% for energy transfer from β-carotene to chlorophyll a in the PS I and in the PS II complexes.