Excitation energy transfer in native and unstacked thylakoid membranes studied by low temperature and ultrafast fluorescence spectroscopy
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- van der Weij-de Wit, C.D., Ihalainen, J.A., van Grondelle, R. et al. Photosynth Res (2007) 93: 173. doi:10.1007/s11120-007-9157-1
In this work, the transfer of excitation energy was studied in native and cation-depletion induced, unstacked thylakoid membranes of spinach by steady-state and time-resolved fluorescence spectroscopy. Fluorescence emission spectra at 5 K show an increase in photosystem I (PSI) emission upon unstacking, which suggests an increase of its antenna size. Fluorescence excitation measurements at 77 K indicate that the increase of PSI emission upon unstacking is caused both by a direct spillover from the photosystem II (PSII) core antenna and by a functional association of light-harvesting complex II (LHCII) to PSI, which is most likely caused by the formation of LHCII-LHCI-PSI supercomplexes. Time-resolved fluorescence measurements, both at room temperature and at 77 K, reveal differences in the fluorescence decay kinetics of stacked and unstacked membranes. Energy transfer between LHCII and PSI is observed to take place within 25 ps at room temperature and within 38 ps at 77 K, consistent with the formation of LHCII-LHCI-PSI supercomplexes. At the 150–160 ps timescale, both energy transfer from LHCII to PSI as well as spillover from the core antenna of PSII to PSI is shown to occur at 77 K. At room temperature the spillover and energy transfer to PSI is less clear at the 150 ps timescale, because these processes compete with charge separation in the PSII reaction center, which also takes place at a timescale of about 150 ps.
KeywordsEnergy transfer LHCII-LHCI-PSI supercomplexes Low-temperature fluorescence Spillover Time-resolved fluorescence Unstacked thylakoid membranes
In green plant photosynthesis, photosystem I (PSI) and photosystem II (PSII) convert light into chemically stored energy. In the light, they work either in series, with plastoquinone conducting the linear electron transport from PSII to PSI, or PSI is involved in cyclic electron transport with the cytochrome b 6 f complex. Both photosystems I and II have a peripheral light harvesting-antenna, called LHCI and LHCII, respectively, which absorb light in partially different regions of the visible spectrum. The electron flow between the two photosystems is optimized by a controlled distribution of excitation energy. Redistribution is realized by a process called state transitions, which is based on a migration of ‘mobile’ LHCII (Murata 1969; Allen and Forsberg 2001; Wollman 2001).
Reversible phosphorylation of LHCII is believed to play an essential role in state-transitions (Dèpege et al. 2003). Upon light illumination favoring PSII a part of LHCII becomes phosphorylated and moves from PSII to PSI, i.e. formation of state 2. A transition to state 1 occurs upon PSI light illumination (or darkness) in which the phosphorylated LHCII becomes dephosphorylated and dissociates from PSI to recombine with PSII again. Phosphorylation and dephosphorylation are under the control of redox sensitive protein kinases and phosphatases present in the photosynthetic membrane (Dèpege et al. 2003). However, a study by Zhang and Scheller (2004) showed that phosphorylation of LHCII is not necessary for its binding to PSI. Photosystem I was found to bind a significant amount of unphosphorylated LHCII in state 2.
Biochemical studies indicated that the PSI-H, -I, -L and -O subunits are involved in the binding of LHCII to PSI (Zhang and Scheller 2004; Lunde et al. 2000; Jensen et al. 2004). The PSI structure of pea (Ben-Shem et al. 2003) shows an empty pocket at the PSI-A, -K and -L units, which was proposed to comprise the docking site for LHCII (Ben-Shem et al. 2004; Dekker and Boekema 2005). Recently, electron microscopy of solubilized thylakoid membranes of Arabidopsis thaliana, prepared either in state 1 or in state 2, revealed the presence of LHCII-LHCI-PSI supercomplexes, which were more abundant in state 2 (Kouril et al. 2005). The 16 Å projection map could be assigned to a specific association of PSI and one LHCII trimer using the structures published by (Ben-Shem et al. 2003) and (Liu et al. 2004), respectively. The LHCII trimer is attached at a defined position between subunits PSI-A, -H, -L and -K. A possible second binding site for an LHCII trimer is pointed out to consist of the subunits PSI -H, -I, -B and -G. The presence of LHCII was confirmed by excitation spectra of the PSI emission of membranes in state 1 and 2 (Kouril et al. 2005).
The thylakoid membrane is composed of successive stacked regions, the grana, interconnected by single membranes or stroma lamellae. The photosystems are known to be inhomogeneously distributed within the thylakoid membrane, with the grana stacks being rich in PSII and LHCII, whereas the stroma lamellae are richly occupied by PSI (Albertsson and Andreasson 2004). Upon cation-depletion, the grana stacks unfold and a so-called bleb is formed. Unstacking of the thylakoid membrane by cation-depletion is known to increase the PSI fluorescence emission (e.g. Barber 1980; Briantais et al. 1984; Williams et al. 1987; Stoitchkova et al. 2006). Both Briantais and co-workers and Stoitchkova and co-workers assigned this increase to spillover from PSII to PSI, as a result of the induced homogeneous distribution of both photosystems by unstacking. Williams and co-workers showed that the presence or absence of Mg2+ ions hardly influences the organization of PSI-LHCI-LHCII sheets. However, in absence of Mg2+ an increased PSI fluorescence was recorded and LHCII to PSI energy transfer observed by fluorescence emission and excitation spectra, similar to a state 1 to state 2 transition (Kouril et al. 2005). Thus it was concluded that it is not the unstacking of the thylakoid membrane, which initiates the increase of the PSI absorption cross-section, but rather a change in electrostatic forces, which drive LHCII apart, and allow them to functionally associate with PSI.
In this study, we show by low temperature steady-state fluorescence measurements that unstacking of the thylakoid membrane results mainly in energy transfer from LHCII to PSI, but also in direct spillover from the PSII core antenna to PSI. The first process may be the result of the formation of LHCII-LHCI-PSI supercomplexes, similar to a state-transition. Time-resolved fluorescence measurements both at room temperature and 77 K, reveal the time constants of both energy transfer processes.
Materials and methods
Stacked thylakoid membranes were prepared from fresh, dark-adapted spinach leaves, obtained from local shops. The leaves were depetiolated and ground in a blender in a buffer containing 50 mM Hepes pH 7.5, 0.4 M NaCl, 2.0 mM MgCl2, 1 mM EDTA and 2 mg/ml bovine serum albumin; washed in a buffer containing 50 mM Hepes pH 7.5, 0.15 M NaCl and 4.0 mM MgCl2; and diluted in a buffer containing 20 mM Hepes pH 7.5, 20 mM NaCl, 5 mM MgCl2. Unstacked thylakoid membranes were prepared as above, but MgCl2 was omitted from all buffers, while the grind buffer also contained 4 mM EDTA (Dekker et al. 2002). At room temperature, 1 mM ferricyanide was added to keep the PSII reaction centers open. Photosystem II membranes or BBY particles were isolated from thylakoid membranes as described by (Berthold et al. 1981) with some modifications as described by (Van Leeuwen et al. 1991) and dissolved in the same buffer as the native membranes. Additionally GY particles (named after Ghanotakis and Yocum who where the first ones to isolate this particle), which consist of the PSII core complex and the minor antenna complexes CP29 and CP26 were prepared as in Ghanotakis et al. (1987). The PSI-LHCI complexes were isolated from unstacked spinach thylakoid membranes as described in Dekker et al. (2002) and diluted in a buffer of 20 mM BisTris pH 6.5, 5 mM MgCl2 and 0.06% of β-DM. For the low temperature fluorescence measurements, 60% (v/v) glycerol was added as cryoprotectant. A nitrogen cryostat (Oxford) was used to cool the samples to 77 K. A helium bath cryostat (Utreks, 4 K) was used to cool the samples to 4 K. The isolated membranes were diluted to an optical density less than 0.1 cm−1 at 680 nm for the steady-state measurements and 0.9 cm−1 for the time-resolved fluorescence measurements.
Fluorescence emission spectra were measured with a 0.5 m imaging spectrograph (Chromex 500IS) and a CCD camera (Chromex Chromcam I). The spectral resolution was 0.15 nm. For broadband excitation a tungsten halogen lamp (Oriel) was used with an interference filter transmitting at 420 nm, bandwidth 15 nm.
Fluorescence excitation spectra were measured with a fluorimeter (Jobin Yvon, FL 3-11). The membranes were excited by a Xenon lamp, with both excitation and detection bandwidth 1 nm. The fluorescence was detected at 735 nm.
The time-resolved measurements were performed with a streak camera. Briefly, 486 nm, vertically polarized excitation pulses of ∼100 fs were generated using a Ti:sapphire laser (VITESSE, Coherent St. Clara, CA) with a regenerative amplifier (REGA, Coherent), a double pass optical parametric amplifier (Coherent, OPA) and a Berek compensator. For the room temperature measurements, the excitation light was collimated with a 15 cm focal length lens, resulting in a focal diameter of 150 μm in the sample. The repetition rate was 200 kHz and the pulse energy 1 nJ. The sample was in a 1 cm polystyrene cuvette and magnetically stirred. For the 77 K measurements, an unfocussed excitation beam was used with a diameter of ∼1 mm. The repetition rate was 50 kHz and the pulse energy 20 nJ. The sample was in a 1 cm polystyrene cuvette in a nitrogen cryostat (Oxford). Both at room temperature and 77 K, the fluorescence was detected in front-face mode at the magic angle, using a Chromex 250IS spectrograph and a Hamamatsu C 5680 synchroscan streak camera. The streak images were recorded with a cooled, Hamamatsu C4880 CCD camera. The full width at half maximum of the overall time response of the experiments was 28 ps at room temperature and 10 ps at 77 K. In the global analysis, both the instrument response and time dispersion were free parameters of the fit.
The datasets obtained with the streak-camera setup, consist of a two-dimensional image of fluorescence intensity as a function of both time and wavelength. Before analysis, the images were corrected for background and sensitivity of the detection system. These images were sliced up into time traces, which span 4 nm and was fit with a sum of exponentials with different decay times. The amplitudes of these exponentials as a function of emission wavelength provide Decay Associated Spectra (DAS) where a positive amplitude represents a loss of fluorescence, whereas a negative amplitude reflects a rise of fluorescence. Hence a DAS with a positive amplitude at short wavelengths and a negative amplitude at higher wavelengths represents an energy transfer process, whereas an overall positive spectrum describes either trapping of excitations by one of the reaction centers or a natural fluorescence emission of the pigments (the latter occurs typically at the ns-time scale). For more details, see (Van Stokkum et al. 2004; Holzwarth 1996).
Using the above approach, the overwhelming numbers of dynamic spectral processes, which take place in the system under study, are described with a few essential/indicative time constants, which describe the main processes of the system. One has to keep in mind, however, that the separation power of the lifetimes is close to a factor of 10 and thus many parallel kinetic processes, which obviously takes place in photosynthetic membranes, may be “lumped” together into one spectrum. Therefore, additional information is required for reliable assignments of the components, which particularly in this case means information from the isolated photosynthetic complexes.
Results and discussion
5 K fluorescence emission
77 K fluorescence excitation
In the same figure, the fluorescence excitation difference spectrum is plotted. This spectrum reveals the origin of the pigments that transfer additional excitation energy to PSI upon unstacking. This spectrum shows peaks at 675 and 650 nm and a shoulder at 672 nm, and largely resembles the absorption spectrum of trimeric LHCII. However, the excitation difference spectrum extends somewhat to the red with respect to the absorption of trimeric LHCII and shows a higher Chl a/b ratio. A combination of fluorescence excitation spectra of the PSII core complex, minor Chl a/b complexes and LHCII was necessary to obtain a satisfactory fit, see Fig. 2. For an estimation of the sum of the first two contributions, fluorescence excitation spectra of GY membranes were used, which consist of the PSII core complex and the minor antenna complexes CP29 and CP26 (Ghanotakis et al. 1987). The GY excitation spectrum accounts for absorption strength in the red flank of the excitation difference spectrum (caused by red Chls in the core antenna proteins CP47 and CP43) and has a higher Chl a/b ratio than LHCII. Because a small amount of PSII fluorescence is recorded at 735 nm (see, e.g., Andrizhiyevskaya et al. 2005) and the amount of PSII fluorescence is higher in native than in unstacked membranes (Fig. 1), a negative contribution of the PSII absorption is expected in the 735 nm excitation difference spectrum of unstacked minus native membranes. The positive contribution of the PSII spectrum (from GY) to the excitation difference spectrum therefore evidences the presence of spillover from PSII to PSI in the unstacked thylakoid membranes.
The excitation spectra of the two types of membranes were fitted with a sum of PSI, GY and LHCII excitation spectra (normalized to their maximum absorbance in the Qy region), resulting in the respective ratios 1:0.19:0.19 in the native membranes and 1:0.36:0.53 in unstacked membranes. We assume that the contributions of GY and LHCII in the excitation spectrum of the native membranes (0.19 each) represent directly excited PSII. This implies that the additional contribution to the fluorescence at 735 nm in the unstacked membranes is caused by excitation energy transfer from the PSII core (GY) and LHCII to PSI. The additional contribution is larger for LHCII (0.34) than for the PSII core (0.17). We conclude that trimeric LHCII accounts for 2/3 of the fluorescence excitation difference spectrum of unstacked minus native membranes. From the fluorescence excitation spectra in Fig. 2, the PSI antenna is estimated to increase with ∼36% of its Chl a upon unstacking of the thylakoid membrane, of which thus ∼24% is due to the functional association of LHCII with PSI. We conclude that there is a significant extent of LHCII to PSI energy transfer, which could, at least in part, originate from the presence of LHCII-LHCI-PSI supercomplexes in the unstacked thylakoid membranes, as in state 2 membranes (Kouril et al. 2005). The remaining part of the energy transfer to PSI may then originate from spillover to PSI from PSII cores, PSII-LHCII supercomplexes or LHCII that is not directly bound to PSII. Both mechanisms result in a decreased PSII emission and increased PSI emission conform our observations in Fig. 1.
Room temperature time-resolved fluorescence
A significant difference between the two types of membranes is displayed by the first DAS (Fig. 3a) which has a lifetime of 18 ps in native and 25 ps in unstacked membranes and which has a much larger amplitude in the unstacked membranes. For the native thylakoid membranes, our data show a fluorescence decay as judged from the overall positive amplitude between 665 nm and 725 nm with an apparent maximum at 686 nm (Fig. 3a). One of the two main trapping phases of PSI-LHCI occurs in 20–30 ps (Ihalainen et al. 2005), originating mainly from excitations in the PSI core complex (Gobets et al. 2001; Gobets and Van Grondelle 2001; Melkozernov et al. 2004). The DAS of this trap peaks around 685 nm and gradually decreases towards red wavelengths, similar to what we observe for the native membranes. The overall equilibration between LHCI and the PSI core proceeds, however, on longer timescales (Ihalainen et al. 2005). We therefore assign the 18 ps DAS to a mixture of trapping in the PSI core and excitation energy equilibration between LHCI and the PSI core complex. The 18 ps phase of the native membranes seems to lack a significant contribution of PSII. This is consistent with an organization of PSII in larger complexes than cores in these conditions, since PSII cores have a major trapping time of about 40 ps (Miloslavina et al. 2006), whereas trapping in PSII membranes occurs on a longer time-scale (Broess et al. 2006). The DAS of the unstacked membranes, extends to the blue with respect to the native DAS, with its maximum at 680 nm, but moreover it shows a small rise of fluorescence around 730 nm. Energy transfer from LHCII trimers to other complexes is expected to occur on this time-range (Barzda et al. 2001; Van Amerongen and Van Grondelle 2001) as well. Thus, the spectrum and amplitude of the 25 ps energy transfer component in the unstacked membranes with the positive feature at 675–680 nm and the negative feature above 720 nm and the absence of these characteristics in the native membranes can be explained by energy transfer from LHCII to PSI in presumably LHCII-LHCI-PSI complexes. The overall larger amplitude of the 25 ps phase in unstacked membranes can be explained by more excitation energy going to PSI and by a larger contribution of trapping in PSII, caused by the occurrence of many PSII complexes as cores in unstacked membranes (Dekker et al. 2002).
An overall positive DAS was resolved with similar lifetimes of 158 and 157 ps in native and unstacked thylakoid membranes, respectively (Fig. 3b). Also this phase is much stronger in unstacked membranes than in native membranes. Both PSI and PSII trap excitation energy by charge separation in their reaction centers at this timescale: PSI-LHCI has been shown to have a second main trapping phase of about 100 ps that is characterized by a redshifted spectrum (Ihalainen et al. 2002, 2005), while the overall excitation decay of PSII in PSII membranes is around 150 ps (Van Mieghem et al. 1992; Broess et al. 2006). As the PSI antenna size has increased at the expense of the PSII antenna in unstacked membranes (see Fig. 1), this DAS is expected to be dominated by PSI trapping for the unstacked membranes, whereas PSII trapping will dominate the native DAS. Indeed, the typical PSI emission decay amplitude around 720 nm is much larger in the unstacked membranes. However, this spectrum also shows a superposed emission decay at 680 nm of similar amplitude as in the native membranes. As the trapping yield will scale with the antenna size, which is smaller in the case of the unstacked membranes, we explain the large contribution at 680 nm to the 157 ps DAS in the unstacked membranes by the occurrence of LHCII to PSI energy transfer as well as spillover at this timescale. Consequently, the PSI trapping amplitude is partially cancelled by the rise of the emission at the same timescale. Support of this interpretation can be found in the next section. Spillover is expected to lead to a decreased PSII trapping timescale because of the competition between these two processes. Absence of this decrease in decay time upon unstacking of the thylakoid membrane—Fig. 3b—suggests that this decay component is dominated by energy transfer from LHCII to PSI in presumably LHCII-LHCI-PSI supercomplexes rather than spillover.
Trapping at longer timescales was resolved with a lifetime of 541 ps for the native membranes and 536 ps for the unstacked membranes (Fig. 3c). This phase is much stronger in the native membranes. It is known that PSI has trapped all absorbed energy within 120 ps (Ihalainen et al. 2002), whereas the overall excitation decay of PSII in PSII membranes occurs on a timescale of 150 ps (Van Mieghem et al. 1992; Broess et al. 2006). Thus, we assign this long phase to the presence of a fraction of closed PSII reaction centers. If the amount of closed centers is similar in both types of membranes, the contribution of this phase is expected to be higher in the native membranes, because more excitations go to PSII with respect to unstacked membranes (Fig. 1).
The fluorescence kinetics of native and unstacked thylakoid membranes of lettuce, with open PSII reaction centers has been compared by (Hodges et al. 1987). As in our study, they found similar decay times among the two membranes—40, 155, 360, and 863 ps for native membranes and 50, 139, 354, and 1,198 ps for unstacked membranes—which differed significantly in yield. In their case, the main difference in yield existed for the ∼150 ps decay, which had a much larger amplitude in case of the unstacked membranes, which is similar to our results (Fig. 3b).
77 K time-resolved fluorescence
The native and unstacked membranes, the BBY membranes and the PSI-LHCI complexes all show a sub-10 ps fluorescence lifetime component. In the PSII spectrum (Fig. 4c) this component has a small positive amplitude around 660 nm, which changes into a negative amplitude above 670 nm, a minimum around 680 nm and about zero amplitude at long wavelengths. This spectral component thus describes energy transfer from Chl b and blue Chl a states to more red Chl a states. In PSI (Fig. 4d), energy equilibration among bulk (685 nm) and red Chls (730 nm) is observed to occur on a similar timescale. In this case, the non-conservativity of the DAS is assigned to the trapping of excitations in the PSI core (Gobets et al. 2001; Ihalainen et al. 2002) on early timescales. The PSI spectrum is negative at long wavelengths, which is also observed in the stacked and unstacked thylakoid membranes, indicating that PSI contributes to the sub-10 ps phase of both. The slightly larger amplitude of the negative contribution around 720 nm and the positive contribution at 670 nm in the unstacked membranes suggests that part of the additional PSI antenna transfers the excitation energy on this sub-10 ps timescale to the red states of PSI.
The second estimated decay component, Fig. 4a and b, has a very similar lifetime for both the native and unstacked thylakoid membranes, 39 and 38 ps, respectively, though the spectra differ clearly. For the native membranes, the resolved 39 ps DAS shows great similarity with the second DAS found in BBY samples (Fig. 4c), which has a decay time of 42 ps. This DAS describes energy transfer, which is observed to be rather conservative in the BBY membranes, with loss of emission at 675 nm, a zero-crossing at 682 nm and a gain at 687 nm. This DAS is interpreted as energy transfer from LHCII to the PSII core complex (Andrizhiyevskaya et al. 2005), where the transfer timescale is in agreement with the 32 ps migration time of excitations between LHCII trimers which was estimated at room temperature (Barzda et al. 2001; Van Amerongen and Van Grondelle 2001). The non-conservativity is explained by trapping taking place on a similar timescale in PSII. The 38 ps DAS of the unstacked membranes (Fig. 4b) is seen to have a broadened and larger positive peak at 677 nm with respect to the 39 ps DAS of the native membranes (Fig. 4a), a zero-crossing at 707 nm and a large negative contribution around 730 nm. The latter contribution can be in part explained by the processes within the PSI-LHCI complex (which shows a rather conservative energy transfer spectrum with positive contributions around 700 nm, a zero-crossing at 720 nm and negative around 740 nm—Fig. 4d), but the large positive band at 677 nm (Fig. 4b) does not occur in isolated PSI complexes and the zero-crossing is much further to the blue. We attribute the 38 ps resolved energy transfer component to a new energy transfer process not present in either PSII membranes or PSI complexes, i.e. the main energy transfer component from LHCII to PSI in LHCII-LHCI-PSI complexes and subsequent energy equilibration with the red pigments.
In BBY membranes PSII was found to trap excitations on a 132 ps timescale (Fig. 4c, maximum at 681 nm). Again, the corresponding DAS of the native membranes (145 ps) shows large spectral similarity with that of BBY, whereas for the unstacked membranes (151 ps) energy transfer from bulk (681 nm) to red pigments (730 nm) is found to occur as well. A 150 ps phase appeared to be absent in PSI (Fig. 4d). We explain the 150 ps resolved energy transfer component in the unstacked membranes by energy transfer from LHCII to PSI and partially by spillover from PSII to PSI. The subsequent equilibration (59 ps—Fig. 4d) and trapping (505 ps—Fig. 4d) in PSI explains the observed non-conservativity in the 150 ps DAS of the unstacked membranes. Note that the 680 nm decay amplitude of this component is only slightly larger for native than for unstacked thylakoid membranes, despite their different PSII antenna size. This suggests that relatively more 680 nm emission disappears in this time domain, which supports the presence of LHCII to PSI energy transfer and spillover (see also Fig. 3b). Again, there is no decrease in fluorescence decay time upon unstacking of the thylakoid membrane, the timescale even increases from 145 to 151 ps, which suggests a dominant contribution of energy transfer from LHCII to LHCI-PSI complexes with respect to spillover to this decay component.
The fourth component has a decay time of 537 ps in case of the native and 673 ps for the unstacked membranes. Both DAS arise as a superposition of the 478 ps PSII trapping in BBY membranes with a spectrum peaking at 687 nm (Fig. 4c) and the 505 ps trapping in PSI with a spectrum peaking at 718 nm (Fig. 4c). Clearly, the ratio in which these respective processes contribute differs among the two types of membranes, with a relatively larger PSI contribution in the case of unstacked membranes as seen from the ratio of amplitudes both at 680 and 720 nm. The increased trapping time in unstacked with respect to native membranes may be a consequence of the increased PSI antenna size by the addition of LHCII.
The redmost pigments in PSI, with their fluorescence maximum at 733 nm (Fig. 4d), decay on both 2.3 and 7.4 ns timescales (Fig. 4d), which is resolved both in the native (3.4 ns) and unstacked membranes (3 ns) (Fig. 4a and b). These DAS will also cover some slow PSII trapping, though the amplitude of the PSII contribution is probably very small (Fig. 4c). The slow trapping phase in BBY membranes—4.8 ns—is seen to have its emission maximum at 693 nm and therefore likely represents trapping on the red pigment(s) of CP47 (Andrizhiyevskaya et al. 2005).
Note that the steady-state emission spectrum arises from the product of the amplitudes and lifetimes of all fluorescence decay phases. For instance, the DAS of BBY (Fig. 4c) show that the band peaking at about 685 nm has a lifetime of about 500 ps and a large amplitude, whereas the band peaking at about 695 nm has a lifetime of about 5 ns but has a much smaller amplitude. This confirms that the two main emission bands of PSII at 77 K (F-685 and F-695) have very different origins (Andrizhiyevskaya et al. 2005). Similarly, the DAS of PSI-LHCI clearly show the presence of two different pools of red pigments, with emission at 718 and 733 nm, which are respectively located in the core complex and light-harvesting antennae (Van Grondelle et al. 1994). The red pigments of the PSI core are seen to become populated in the early timescale (9 ps), whereas the emission from the red pigments in LHCI arises relatively slowly at the timescale of 59 ps (Fig. 4d).
Upon cation-depletion, native thylakoid membranes will unstack. We present here a combined study of low temperature fluorescence emission and excitation and show that LHCII is partially released from PSII upon unstacking of the thylakoid membrane and that a part of the LHCII functionally associates with PSI, most likely in the form of LHCII-LHCI-PSI supercomplexes. Time-resolved fluorescence measurements at room temperature reveal energy transfer from LHCII to PSI to take place on a timescale of 25 ps, which is somewhat longer at 77 K (38 ps), consistent with the organization in an LHCII-LHCI-PSI supercomplex. A second estimated timescale for energy transfer from LHCII to PSI—150–160 ps—will originate from energy transfer from LHCII which is less tightly associated with an LHCI-PSI complex than LHCII which transfers energy to LHCI-PSI on a 30 ps timescale, or perhaps from a second LHCII trimer bound to an LHCII-LHCI-PSI supercomplex. Spillover from PSII to PSI was found to take place at the same timescale (150–160 ps) also both at room temperature and 77 K, which is the same timescale on which trapping occurs in PSII in intact membranes. Our results suggest that cation depletion induces direct energy transfer from LHCII to PSI and therefore at least partially mimics a state transition.
We thank I.H.M. van Stokkum for help in global analysis. This work was supported by the Netherlands Organization for Scientific Research (NWO) by a grant from the Foundation for Fundamental Research on Matter (FOM), and by the European Union by a grant to the PSICO Research Training Network (HPRN-CT-2002-00248) and the Intro2 Marie Curie Research Training Network (MRTN-CT-2003-505069).