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First published online November 14, 2008; 10.1104/pp.108.129957

Plant Physiology 149:1061-1075 (2009)
© 2009 American Society of Plant Biologists

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BIOENERGETICS AND PHOTOSYNTHESIS

The Zeaxanthin-Independent and Zeaxanthin-Dependent qE Components of Nonphotochemical Quenching Involve Common Conformational Changes within the Photosystem II Antenna in Arabidopsis1,[W]

Matthew P. Johnson, María L. Pérez-Bueno, Ahmad Zia, Peter Horton and Alexander V. Ruban*

School of Biological and Chemical Sciences, Queen Mary University of London, London E1 4NS, United Kingdom (M.P.J., A.Z., A.V.R.); and Department of Molecular Biology and Biotechnology, University of Sheffield, Sheffield S10 2TN, United Kingdom (M.L.P.-B., P.H.)


    ABSTRACT
 TOP
 ABSTRACT
 RESULTS
 DISCUSSION
 MATERIALS AND METHODS
 LITERATURE CITED
 
The light-harvesting antenna of higher plant photosystem II (LHCII) has the intrinsic capacity to dissipate excess light energy as heat in a process termed nonphotochemical quenching (NPQ). Recent studies suggest that zeaxanthin and lutein both contribute to the rapidly relaxing component of NPQ, qE, possibly acting in the minor monomeric antenna complexes and the major trimeric LHCII, respectively. To distinguish whether zeaxanthin and lutein act independently as quenchers at separate sites, or alternatively whether zeaxanthin fulfills an allosteric role regulating lutein-mediated quenching, the kinetics of qE and the qE-related conformational changes ({Delta}A535) were compared in Arabidopsis (Arabidopsis thaliana) mutant/antisense plants with altered contents of minor antenna (kolhcb6, aslhcb4), trimeric LHCII (aslhcb2), lutein (lut2, lut2npq1, lut2npq2), and zeaxanthin (npq1, npq2). The kinetics of the two components of NPQ induction arising from zeaxanthin-independent and zeaxanthin-dependent qE were both sensitive to changes in the protein composition of the photosystem II antenna. The replacement of lutein by zeaxanthin or violaxanthin in the internal Lhcb protein-binding sites affected the kinetics and relative amplitude of each component as well as the absolute chlorophyll fluorescence lifetime. Both components of qE were characterized by a conformational change leading to nearly identical absorption changes in the Soret region that indicated the involvement of the LHCII lutein 1 domain. Based on these observations, we suggest that both components of qE arise from a common quenching mechanism based upon a conformational change within the photosystem II antenna, optimized by Lhcb subunit-subunit interactions and tuned by the synergistic effects of external and internally bound xanthophylls.


The chlorophyll a/b-binding light-harvesting antenna of photosystem II (PSII of higher plants is responsible for the efficient collection and transfer of excitation energy to the reaction center. The PSII antenna comprises the main trimeric light-harvesting complex, LHCII, which is composed of the Lhcb1 to -3 polypeptides, and the minor light-harvesting complexes, CP29, CP26, and CP24, composed of Lhcb4, -5, and -6, respectively. In Arabidopsis (Arabidopsis thaliana), four LHCII trimers associate with two copies each of CP24, CP26, and CP29 and a core dimer of PSII (CP43/D1/D2/CP47) to form the C2S2M2 LHCII-PSII supercomplex (Dekker and Boekema, 2005Go). In addition, depending upon the growth conditions, two or three extra LHCII trimers per PSII may be present in LHCII-only regions of the grana, providing additional light-harvesting capacity.

The PSII antenna is a highly dynamic system that is able to tune the amount of excitation delivered to the PSII reaction center to match physiological need (Horton et al., 1996Go). The regulation of energy flow occurs by control of the thermal dissipation of excess excitation within the PSII antenna, a process termed nonphotochemical quenching (NPQ). NPQ is heterogeneous, comprising a slowly reversible qI component and a rapidly reversible qE component (Horton et al., 1996Go). The trigger for qE is the buildup of the transmembrane proton gradient or {Delta}pH (Briantais et al., 1979Go). The {Delta}pH is sensed by the PsbS protein (Li et al., 2004Go), without which the rapidly reversible behavior of NPQ is lost (Li et al., 2000Go). Full expression of qE in vivo is associated with the enzymatic deepoxidation of the epoxy-xanthophyll violaxanthin to zeaxanthin, via the action of the xanthophyll cycle (Demmig-Adams, 1990Go). The majority of the photoconvertible xanthophyll cycle pool is associated with trimeric LHCII, bound at the external V1 binding site (Ruban et al., 1999Go, 2002aGo; Caffarri et al., 2001Go; Liu et al., 2004Go). Trimeric LHCII binds two other types of xanthophylls internally: two all-trans-luteins at the L1 and L2 sites associated with the central membrane-spanning {alpha}-helices; and a 9-cis-neoxanthin at the N1 site associated with the C-helix chlorophyll b domain (Liu et al., 2004Go). The minor monomeric complexes CP24, CP26, and CP29 all bind lutein at the L1 site. In addition, CP29 binds two xanthophyll cycle carotenoids and one-half to one neoxanthin, CP24 binds two xanthophyll cycle carotenoids, while CP26 binds one xanthophyll cycle carotenoid and one neoxanthin (Peter and Thornber, 1991Go; Bassi et al., 1993Go; Ruban et al., 1994Go, 1999Go; Morosinotto et al., 2002Go).

Although there is strong evidence that qE occurs in the PSII antenna light-harvesting proteins and that xanthophylls are involved, the mechanism of energy dissipation remains unclear. There is evidence for two distinct quenching mechanisms, one involving zeaxanthin (type I) and the other lutein (type II). In the type I mechanism, it is proposed that qE obligatorily depends upon zeaxanthin acting as a quencher of excited chlorophyll via the formation of a charge transfer state. Evidence for type I is the formation of a carotenoid radical cation absorbing at approximately 1,000 nm that correlates with the extent of qE (Holt et al., 2005Go). Recently, evidence was obtained that formation of the zeaxanthin radical cation occurs exclusively at the L2 binding site of the minor antenna complexes (Ahn et al., 2008Go; Avenson et al., 2008Go), quenching therefore requiring reversible insertion of zeaxanthin into this internal site. Because the effect of this cation on the excited-state lifetime of the minor antenna complexes was found to be very small, it was suggested that in vivo, under the influence of the {Delta}pH, a large population of complexes would adopt a conformation in which this species could form (Avenson et al., 2008Go). Evidence was also obtained that a zeaxanthin radical cation may form in trimeric LHCII (Amarie et al., 2007Go). Again, the effect on the chlorophyll excited-state lifetime was very small, leading these authors to conclude that the type I mechanism could not be responsible for qE (Amarie et al., 2007Go; Dreuw and Wormit, 2008Go).

In the type II mechanism, qE is an inbuilt property of LHCII proteins; a protein conformational change alters the configuration of bound pigments and results in the xanthophyll bound at the L1 site (normally lutein) becoming an effective quencher of chlorophyll excited states (Ruban et al., 2007Go; Ilioaia et al., 2008Go). Evidence for a type II mechanism came from studies of trimeric LHCII aggregates (Ruban et al., 2007Go). Here, it was concluded that energy dissipation occurs by energy transfer from chlorophyll a to the S1 state (2Ag1) of lutein bound at the L1 site. Notably, this quenching mechanism decreases the chlorophyll excited-state lifetime by a magnitude sufficient to fully account for qE in vivo. A change in the conformation of another LHCII-bound xanthophyll (neoxanthin) correlates with the extent of quenching. This conformational change takes place in vivo with an amplitude that correlates with the amount of qE. In the model for type II quenching proposed by Horton and coworkers (1991Go, 2005Go), zeaxanthin acts not as a quencher but as an allosteric modulator of the {Delta}pH sensitivity of this intrinsic LHCII quenching process.

Although the type I and type II mechanisms involve different xanthophylls operating at different sites, there are similarities: in particular, both are proposed to involve a {Delta}pH-triggered, PsbS-mediated conformational change (Ruban et al., 2007Go; Ahn et al., 2008Go). Indeed, it is possible that both mechanisms contribute to in vivo qE, since the process occurs in both the presence and absence of zeaxanthin (Adams et al., 1990Go; Crouchman et al., 2006Go). The crucial question is whether zeaxanthin-dependent and zeaxanthin-independent qE arise from the same mechanism (type II) or from two different ones (types I and II, respectively). The kinetics of NPQ formation upon the illumination of dark-adapted leaves comprise two components: the first forms rapidly and is zeaxanthin independent; the second, slower component correlates with violaxanthin deepoxidation and therefore is described as zeaxanthin dependent (Adams et al., 1990Go; Ruban and Horton, 1999Go). The two components of NPQ formation are of the qE type: both relax rapidly upon darkening (Adams et al., 1990Go); both are dependent upon PsbS (Li et al., 2000Go); and both are enhanced by PsbS overexpression (Li et al., 2002Go; Crouchman et al., 2006Go). Investigation of these kinetics provides an opportunity to determine whether a single mechanism can account for qE and to give clues to which type of mechanism is involved. Here, we test the hypothesis that the two components arise from different mechanisms: the zeaxanthin-dependent component arising in the minor monomeric antenna by a type I mechanism (Gilmore et al., 1998Go; Ahn et al., 2008Go; Avenson et al., 2008Go), and the zeaxanthin-independent component arising in the major trimeric LHCII by the type II mechanism. An alternative explanation for zeaxanthin-independent qE, at least under low-light conditions, when qE forms transiently, is that it is caused by quenching in the PSII reaction center (Finazzi et al., 2004Go). Several predictions emerge from this hypothesis. First, the removal of certain Lhcb proteins by mutation would differentially affect the two components of qE. Second, because the two components would be additive and could not compensate for the loss of one another (Niyogi et al., 1998Go; Pogson et al., 1998Go), they should each contribute a discrete component to the kinetics of qE formation and relaxation. Third, in mutants lacking lutein, the capacity of the type II mechanism would be reduced, while the zeaxanthin-dependent component would be unaffected. Finally, the two components may be expected to be characterized by different absorption changes in the Soret region, which reflect changes in the absorption spectra of bound pigments brought about by conformational changes within the PSII antenna upon qE formation (Ruban et al., 1993aGo, 1993bGo, 2002bGo; Bilger and Björkman, 1994Go). We tested this hypothesis by analysis of qE kinetics, fluorescence lifetimes, and qE-related absorption difference spectra. Contrary to the above predictions, the data indicated that both steady-state and transient qE arise from a common mechanism within the PSII antenna, in both the presence and absence of zeaxanthin.


    RESULTS
 TOP
 ABSTRACT
 RESULTS
 DISCUSSION
 MATERIALS AND METHODS
 LITERATURE CITED
 

Both Zeaxanthin-Independent and Zeaxanthin-Dependent Components of qE Are Sensitive to Changes in the Protein Composition of the PSII Antenna

NPQ was analyzed in dark-adapted plants lacking the proteins of the major trimeric LHCII (aslhcb2; Andersson et al., 2003Go) and of the minor complexes, CP24 and CP29 (kolhcb6 and aslhcb4, respectively; Andersson et al., 2001Go; Kovacs et al., 2006Go). Analyses of the pigment compositions of the dark-adapted mutant and wild-type leaves indicated no major differences between them, as reported previously (Andersson et al., 2001Go, 2003Go; Kovacs et al., 2006Go; Table I). These mutant/antisense plants also possess unchanged levels of {Delta}pH compared with wild-type plants (Pérez-Bueno et al., 2008Go). The kinetics of NPQ, therefore, should be affected only by the differences in Lhcb protein content. The actinic light intensity of 700 µmol photons m–2 s–1 was carefully selected in order to maximize the qE component of NPQ while minimizing slowly reversible photoinhibitory components. In aslhcb2, the kinetics were considerably slower and the maximum amplitude of NPQ was 67% of that of the wild type (Fig. 1A ; Table II ). A similar result was found in aslhcb4, where the NPQ also formed more slowly than in the wild type and with reduced amplitude (Fig. 1A; Table II). In contrast, in kolhcb6, the formation of NPQ was faster but the final amplitude was only 60% of that found in the wild type (Fig. 1A; Table II).


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Table I. Pigment composition of wild-type and Lhcb mutant plants

Samples were taken from leaves either dark adapted for 30 min or after 10 min of illumination at 700 µmol photons m–2 s–1. Data are normalized to 100 chlorophyll a + b molecules and are means ± SE from four replicates. Neo, Lut, Vio, Ant, Zea, DEPs, and chl a/b represent neoxanthin, lutein, violaxanthin, antheraxanthin, zeaxanthin, deepoxidation state % [(zeaxanthin + 0.5 antheraxanthin)/(violaxanthin + antheraxanthin + zeaxanthin)], and chlorophyll a/b ratio, respectively.

 

Figure 1
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Figure 1. Kinetics of NPQ at 700 µmol photons m–2 s–1 in wild-type and Lhcb mutant leaves dark adapted for 30 min. NPQ formation kinetics (A and B) and NPQ relaxation kinetics (C and D) are shown for the wild type (black stars), aslhcb2 (white triangles), aslhcb4 (white circles), kolhcb6 (black squares), aslhcb4 + DTT (black circles), kolhcb6 + DTT (white squares), aslhcb2 + DTT (black triangles), and the wild type + DTT (white stars). Data are averages of three experiments ± SE.

 

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Table II. Kinetic parameters of NPQ in wild-type and Lhcb mutant plants

Average NPQ formation data were fitted in all cases with a Hill function (y = [axb]/[cb + xb]); data are averages of three independent experiments ± SE. Average NPQ relaxation data were fitted in all cases with a hyperbolic decay (y = y0 + [ab]/[b + x]); data are averages of three independent experiments ± SE. Data were obtained as for Figures 1 (dark adapted) and 3 (preilluminated).

 
To test whether the zeaxanthin-independent or zeaxanthin-dependent components of qE were affected in the Lhcb mutant/antisense plants, the kinetics of NPQ were recorded after infiltration of leaves with dithiothreitol (DTT). HPLC analysis of the leaves revealed no detectable increase in the contents of antheraxanthin or zeaxanthin compared with the dark-adapted leaves, indicating that DTT had completely inhibited deepoxidation (Table I). In wild-type leaves infiltrated with DTT, NPQ formed rapidly, but to a level only 40% of that found in untreated leaves (Fig. 1B). As was the case in the noninfiltrated leaves, in the presence of DTT, rates of NPQ formation in aslhcb2 and aslhcb4 were slower than in the wild type but faster than in kolhcb6 (Fig. 1B; Table II). Significantly, in the presence of DTT, the amplitude of NPQ in each of the mutant/antisense plants was less than in the wild type. Furthermore, the amplitude of the zeaxanthin-dependent NPQ (calculated by the subtraction of NPQ + DTT from the total NPQ [Adams et al., 1990Go]) was also reduced in each mutant. Hence, both the zeaxanthin-dependent and zeaxanthin-independent components of NPQ were sensitive to changes in the PSII antenna protein composition, irrespective of whether the mutation/antisense affected the major trimeric or minor monomeric antenna complexes.

The relaxation of the qE component of NPQ was also monitored in the wild-type and mutant/antisense leaves in both the presence and absence of DTT. qE relaxed with similar kinetics in the wild type and in aslhcb4, but it relaxed more slowly in aslhcb2 and more rapidly in kolhcb6 (Fig. 1, C and D; Table II). In all cases, the relaxation of qE was faster in the presence of DTT, but most importantly, the differences between the mutant/antisense leaves and wild-type leaves were still observed. In all cases, the major fraction of the zeaxanthin-independent NPQ was rapidly reversible (Fig. 1D), showing it to be of the qE type.

The kinetics of the reformation of NPQ were tested in wild-type and mutant/antisense leaves that had previously been preilluminated for 10 min at 700 µmol photons m–2 s–1, before being given 5 min of dark to relax qE. In the wild type and each mutant, the NPQ formation kinetics were accelerated compared with the first illumination cycle (Fig. 2A ; Table II), yet the differences between them were maintained. The aslhcb4 and aslhcb2 formed NPQ more slowly than the wild type, while in kolhcb6 NPQ formed faster. A similar result was also observed for DTT-infiltrated leaves (Fig. 2B; Table II), but interestingly, NPQ now formed more slowly than in noninfiltrated leaves, except in the case of kolhcb6, where there was no difference between the two conditions. Therefore, differences in Lhcb protein composition affect in the same way the formation and relaxation of qE both in the presence and in the absence of deepoxidation.


Figure 2
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Figure 2. Kinetics of NPQ formation at 700 µmol photons m–2 s–1 in wild-type and Lhcb mutant leaves previously preilluminated for 10 min and then dark adapted for 5 min. A, The wild type (black stars), aslhcb2 (white triangles), aslhcb4 (white circles), and kolhcb6 (black squares). B, aslhcb4 + DTT (black circles), kolhcb6 + DTT (white squares), aslhcb2 + DTT (black triangles), and the wild type + DTT (white stars). Data are averages of three experiments ± SE.

 
Investigation of the rate of zeaxanthin formation and comparison with the rate of formation of NPQ allows the sensitivity of NPQ to zeaxanthin in each mutant to be determined. The change in absorption at 505 nm measured relative to a 565-nm reference ({Delta}A505-565) has a linear dependence on zeaxanthin concentration (Bilger et al., 1989Go). Therefore, the kinetics of {Delta}A505-565 following illumination of dark-adapted leaves were monitored (Fig. 3A ). The rate of zeaxanthin formation was significantly faster in kolhcb6 (half-time [t1/2] = 140 ± 4 s) than in either the wild type (t1/2 = 170 ± 4 s) or aslhcb4 (t1/2 = 170 ± 2 s), but in aslhcb2 leaves the kinetics were much slower (t1/2 = 245 ± 8 s). In each case, the deepoxidation states were maximal within approximately 10 min, further illumination producing no additional zeaxanthin formation (data not shown). HPLC analysis of pigments extracted from illuminated plants revealed that the final deepoxidation states were 42% in aslhcb2, 45% in aslhcb4, 46% in the wild type, and 53% in kolhcb6 (Table I). When the kinetics of NPQ formation were plotted against the 505-nm absorption kinetics for the wild-type plants, a nonlinear relationship was found, which may be attributed to the zeaxanthin-independent component of NPQ. Subtraction of the zeaxanthin-independent component of NPQ (wild type minus wild type + DTT [Adams et al., 1990Go]) yields the relationship between zeaxanthin formation and the zeaxanthin-dependent component of NPQ. In the wild type, this relationship was initially linear, as found previously (Demmig-Adams et al., 1989Go), but saturated at high concentrations of zeaxanthin (Fig. 3B). This procedure was repeated for the mutant plants. In the case of aslhcb4, the nonlinearity at high zeaxanthin content was slightly more pronounced. In aslhcb2, the slope of the NPQ versus {Delta}A505-565 plot was significantly reduced, indicating an apparently reduced sensitivity of NPQ to zeaxanthin. In contrast, the kolhcb6 mutant appeared to be initially the most sensitive to zeaxanthin, but the NPQ response was saturated at relatively low levels of zeaxanthin. Thus, changes in the composition of the proteins of both trimeric LHCII and the minor antenna complexes affect the sensitivity of NPQ to zeaxanthin, implicating a role for both sets of proteins in the zeaxanthin-dependent component of qE.


Figure 3
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Figure 3. Kinetics of zeaxanthin formation ({Delta}A505) at 700 µmol photons m–2 s–1 in wild-type (WT) and Lhcb mutant leaves dark adapted for 30 min. A, Eight to 10 kinetic traces were averaged (error ± 10%). B, Relationship between zeaxanthin-dependent phase of NPQ formation (total NPQ kinetics minus NPQ kinetics + DTT) and zeaxanthin formation ({Delta}A505) for the wild type (black stars), aslhcb2 (white triangles), aslhcb4 (white circles), and kolhcb6 (black squares).

 

qE-Related Conformational Changes in the PSII Antenna Are Dependent upon Lhcb Subunit Composition

The formation of qE is correlated with a positive absorption change in leaves at 535 nm ({Delta}A535), which monitors a conformational change within the PSII antenna that accompanies quenching (Heber, 1969Go; Bilger and Björkman, 1990Go; Ruban et al., 1993bGo, 2002bGo; Bilger and Björkman., 1994Go). It would be predicted that the conformational change would be affected by changes in the composition of Lhcb proteins. Figure 4A shows the light-dependent changes in {Delta}A535 recorded for wild-type and mutant/antisense plants. In all plants, the absorption increased upon illumination and relaxed in darkness to a level that was approximately 15% of the maximum amplitude during actinic illumination. A second illumination cycle caused a much faster rise in {Delta}A535 in the wild type. {Delta}A535 increased more slowly in aslhcb4 and aslhcb2 compared with the wild type and with smaller amplitude (85% and 72% of wild-type values, respectively). A second illumination cycle caused an acceleration of {Delta}A535 in aslhcb4 and aslhcb2, yet the signal amplitude was still smaller than in the wild type. Hence, the essential kinetic features of NPQ were reproduced in the {Delta}A535 kinetics, with differences between the plant types observed in a manner consistent with the differences in NPQ kinetics described above. {Delta}A535 formation kinetics in kolhcb6 were very different: {Delta}A535 increased rapidly, reaching a level approximately 15% larger than in the wild type within 60 s, but it subsequently decayed over the next 200 s to a lower amplitude (55% of wild-type values; Fig. 4A). A somewhat smaller transient rise in {Delta}A535 was seen in the second illumination cycle for kolhcb6 (Fig. 4A).


Figure 4
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Figure 4. Light-dependent kinetics of qE-related {Delta}A535 conformational changes at 700 µmol photons m–2 s–1 and qE absorption difference spectra of wild-type and Lhcb mutant leaves dark adapted for 30 min. A and C, Kinetics of {Delta}A535, with traces as labeled. Six to 10 kinetic traces were averaged (error ± 5%). B and D, qE absorption difference spectra (5 min of light minus 5 min of dark relaxation) for the wild type (WT; solid line), aslhcb4 (long dashed line), aslhcb2 (short dashed line), kolhcb6 (dashed dotted line), the wild type + DTT (solid line), kolhcb6 + DTT (dashed dotted line), aslhcb2 + DTT (short dashed line), and aslhcb4 + DTT (long dashed line).

 
Absorption difference spectra (5 min of light minus 5 min of dark relaxation) were recorded in the Soret region (420–565 nm) to provide information on the pigment changes resulting from the qE-related conformational changes (Fig. 4B). In the wild type, the difference spectrum was similar to that reported previously (Ruban et al., 1993bGo), with a broad positive band at 535 nm, attributed to zeaxanthin (Ruban et al., 2002bGo), and negative bands at 495, 468, and 438 nm. The same bands were found in the difference spectra obtained from the kolhcb6, aslhcb2 and aslhcb4 plants, but they were of smaller amplitude, consistent with their reduced levels of qE. In the case of the kolhcb6 mutant, an attempt was made to record a second difference spectrum for the transient signal (1 min of light minus 5 min of dark relaxation). Although it was impossible to obtain a completely accurate spectrum during the transient changes in absorption, a positive band in the 535-nm region and negative bands below 500 nm were observed, the same features found in the steady-state spectrum (data not shown).


Similar Conformational Changes Accompany Both Zeaxanthin-Dependent and Zeaxanthin-Independent Components of qE

Inhibition of zeaxanthin formation by treatment with DTT resulted in a reduction in the amplitude of {Delta}A535 in all plants (Fig. 4C). {Delta}A535 formed rapidly in the wild type, but it was of lower amplitude than in the untreated plants, as reported previously (Bilger and Björkman, 1990Go; Crouchman et al., 2006Go). {Delta}A535 also relaxed faster in the presence of DTT; hence, the kinetic features of {Delta}A535 again matched those of NPQ, even in the absence of zeaxanthin. In aslhcb2 + DTT and aslhcb4 + DTT, the kinetics of {Delta}A535 were slower and the signal was of lower amplitude, approximately 70% of wild-type + DTT levels. Interestingly, when kolhcb6 leaves were infiltrated with DTT, the {Delta}A535 transient seen in untreated leaves was absent and the signal amplitude was smaller than in the wild type.

Absorption difference spectra revealed the nature of the absorption changes that accompany the zeaxanthin-independent component of qE. All of the features present in the difference spectra in untreated leaves were found, although the amplitudes of all bands were smaller, consistent with the reduced level of NPQ in the absence of zeaxanthin (Fig. 4D). The peak position of the positive band was down-shifted from 535 to 525 nm, as reported previously (Noctor et al., 1993Go). The absorption difference spectra in aslhcb2, aslhcb4, and kolhcb6 mutants treated with DTT contained the same bands as in the wild type, but they were smaller in amplitude, consistent with the lower NPQ in these plants. Clearly, both the zeaxanthin-independent and zeaxanthin-dependent components of qE were accompanied by nearly identical conformational changes. Furthermore, these conformational changes are affected by changes in content of both the major trimeric LHCII and minor monomeric components in the PSII antenna.


Absence of Lutein Disrupts the Kinetics and Amplitude of qE

The effect of varying xanthophyll composition within the PSII antenna on the kinetics of the two components of qE was examined in wild-type and xanthophyll mutant leaves. The pigment composition in light-treated and dark-adapted leaves of these mutants (Table III ) was similar to the previously reported values (Niyogi et al., 1998Go; Havaux et al., 2004Go; Pérez-Bueno and Horton, 2008Go). Thus, npq1 and lut2npq1 had no light-induced deepoxidation, whereas npq2 and lut2npq2 had constitutively 100% deepoxidation. In the latter mutant, zeaxanthin also replaces lutein in the internal Lhcb protein-binding sites, whereas in lut2 and lut2npq1, these sites are mostly occupied by violaxanthin. The level of {Delta}pH in these mutants is unchanged compared with the wild type (Pérez-Bueno et al., 2008Go). As before, NPQ formation was measured during two successive periods of illumination. During the first illumination, the well-known differences in the kinetics of NPQ formation were observed (Niyogi et al., 1998Go, 2001Go; Pogson et al., 1998Go). NPQ formed more rapidly in npq2, lut2npq2, and npq1 than in the wild type but was of lower amplitude, while NPQ formation in lut2 was slower (Fig. 5A ; Table IV ). The rates of zeaxanthin formation were virtually identical in lut2 and wild-type plants (data not shown), as found previously (Lokstein et al., 2002Go), indicating that the difference in rates of NPQ formation was due to another factor. In lut2npq1, NPQ was very small and irreversible, indicating the inhibition of zeaxanthin-independent qE in the absence of lutein. Thus, the slower NPQ formation in lut2 compared with the wild type could similarly be due to the absence of zeaxanthin-independent qE.


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Table III. Pigment composition of wild-type and xanthophyll mutant plants

Samples were taken from leaves either dark adapted for 30 min or after 10 min of illumination at 700 µmol photons m–2 s–1. Data are normalized to 100 chlorophyll a + b molecules and are means ± SE from four replicates. Abbreviations are as in Table I. No differences were detected for npq2, npq1, lut2npq1, and lut2npq2 between light and dark conditions (data not shown). Neo, Lut, Vio, Ant, Zea, DEPs, and chl a/b represent neoxanthin, lutein, violaxanthin, antheraxanthin, zeaxanthin, deepoxidation state % [(zeaxanthin + 0.5 antheraxanthin)/(violaxanthin + antheraxanthin + zeaxanthin)], and chlorophyll a/b ratio, respectively.

 

Figure 5
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Figure 5. Kinetics of NPQ at 700 µmol photons m–2 s–1 in wild-type and xanthophyll mutant leaves. A, NPQ formation kinetics in leaves dark adapted for 30 min. B, NPQ formation kinetics in leaves preilluminated for 10 min and then dark adapted for 5 min. C, NPQ relaxation kinetics in leaves dark adapted for 30 min. Plant types are the wild type (black stars), npq2 (white circles), npq1 (black triangles), lut2 (black squares), lut2npq1 (white squares), and lut2npq2 (white diamonds). Data are averages of three experiments ± SE.

 

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Table IV. Kinetic parameters of NPQ in wild-type and xanthophyll mutant plants

Average NPQ formation data were fitted in all cases with a Hill function (y = [axb]/[cb + xb]); data are averages of three independent experiments ± SE. Average NPQ relaxation data were fitted in all cases with a hyperbolic decay (y = y0 + [ab]/[b + x]); data are averages of three independent experiments ± SE. Data were obtained as for Figure 5.

 
Upon the second illumination, qE formed rapidly in the wild-type leaves, reaching saturation in less than 20 s (Fig. 5B; Table IV), and was now faster than that observed in the npq1 mutant. In contrast, npq2 still displayed faster kinetics of NPQ formation than the wild type (Fig. 5B; Table IV). The effect of lutein replacement on qE was dramatic: qE formed more slowly and with reduced amplitude in lut2npq2 compared with npq2. Similarly, the replacement of lutein by violaxanthin in lut2 reduced the rate and amplitude of qE formation compared with the wild type, despite the fact that the deepoxidation state was similar to that in the wild type (Fig. 5B; Table IV). Hence, the replacement of lutein in the internal binding sites of the Lhcb proteins by either violaxanthin or zeaxanthin resulted in a reduction in the rate and amplitude of qE formation independent of differences in the deepoxidation state. It was also tested whether the qE transiently formed at low light intensity, which is suggested to occur in the PSII reaction center (Finazzi et al., 2004Go), was similarly affected by alteration in the xanthophyll composition. The same dependence on xanthophyll composition was found for transient qE occurring at low light intensity as for the steady-state qE generated at high light intensity, with strong reductions in amplitude observed in the npq1, lut2, and lut2npq2 mutants and a complete absence in the lut2npq1 mutant (Supplemental Fig. S1).

The lower values of NPQ in the two zeaxanthin-accumulating mutants have been suggested to arise from the prequenching of Fm (for definitions of fluorescence terms, see "Materials and Methods") caused by sustained zeaxanthin-mediated NPQ (Dall'Osto et al., 2005Go; Kalituho et al., 2006bGo). The presence of such prequenching was supported by the lower Fv/Fm values for dark-adapted npq2 and lut2npq2 plants compared with wild-type plants (Table V ). Chlorophyll fluorescence lifetimes were recorded when all PSII reaction centers were closed by saturating light (Fm) in the presence the uncoupler nigericin to prevent qE formation. The average fluorescence lifetime for dark-adapted wild-type leaves was 2.0 ns, consistent with previously reported values (Gilmore et al., 1998Go). The average fluorescence lifetimes at Fm in dark-adapted npq2 and lut2npq2 leaves were shorter than in the wild type, 1.73 and 1.52 ns, respectively, confirming the presence of prequenching (Table V). The respective Fm' lifetimes in the presence of NPQ were also measured in wild-type leaves: a lifetime of 621 ps was found for leaves with an NPQ value of 2.2, similar to that found previously (Gilmore et al., 1998Go). The fluorescence lifetime in the NPQ state was slightly longer in the npq2 mutant (637 ps with an NPQ of 1.8) but significantly longer in the lut2npq2 mutant (724 ps with an NPQ of 0.95; Table V). Thus, the final extent of quenching in npq2 is similar to that in the wild type, proving that the decrease in observed NPQ is due to prequenching and not to any lesion in NPQ formation. In contrast, in lut2npq2, the final extent of quenching is much less, showing that there is a real reduction in the amplitude of NPQ in this mutant.


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Table V. Average chlorophyll fluorescence lifetimes and Fv/Fm in wild-type and zeaxanthin-accumulating mutant plants

Average Fm and Fm' state lifetimes of dark-adapted leaves from wild-type and xanthophyll mutant plants under saturating light. Data are means ± SE from 10 replicates.

 

qE Relaxation Kinetics Are Composed of a Single Component and Are Modulated by Zeaxanthin

The kinetics of qE relaxation were also analyzed in the xanthophyll mutants. In all cases, the relaxation could be fitted to a single hyperbolic decay (Fig. 5C; Table IV). The rate of relaxation of qE in the npq1 mutant, which contains only the zeaxanthin-independent component of qE, was twice as fast as in the wild type. The comparison of npq1 with npq2 relaxation kinetics provided clues about whether one or two mechanisms are involved in qE. In the case of npq2, if separate type I and type II mechanisms were present, then qE should have relaxed with two components, one of which is fast (as in npq1) and the second of which is slower (because of the presence of zeaxanthin). In contrast to this prediction, it was observed that the additional zeaxanthin in npq2 slowed the relaxation of all of qE, and not just the zeaxanthin-dependent component. Indeed, the rate of relaxation of qE in npq2 was found to nearly triple that found in the wild type (Fig. 5C; Table IV). The replacement of lutein by additional zeaxanthin in lut2npq2 was associated with a further slowing of the relaxation of qE. In contrast, the relaxation of qE in lut2 was marginally faster than in the wild type (Fig. 5C; Table IV). Hence, the amount of zeaxanthin appeared to modulate the rate of qE relaxation, which behaved kinetically as a single process.


qE-Related Conformational Changes Are Dependent upon the Xanthophyll Composition

The qE-related conformational changes were investigated in dark-adapted leaves of wild-type and xanthophyll mutant plants by measurement of the kinetics of {Delta}A535 (Fig. 6A ). Comparison of the wild-type kinetics with those of npq1 confirms that the amplitude of {Delta}A535 is affected by the deepoxidation state; hence, the lower level of qE in this mutant is accompanied by a similarly smaller amplitude of {Delta}A535. The formation of {Delta}A535 was faster in npq2 than in the wild type, while relaxation in the dark was slower, again consistent with the differences observed in the qE kinetics (Fig. 6A). Interestingly, the amplitude of {Delta}A535 in npq2 was as large as in wild-type leaves, whereas qE was less. The complete absence of the {Delta}A535 signal in the lut2npq1 mutant, which displayed no qE, confirms that the signal is only related to qE (Fig. 6B), consistent with data obtained in the npq4 mutant lacking PsbS (Li et al., 2000Go; Ruban et al., 2002bGo). {Delta}A535 formed faster in lut2npq2 than in the wild type and relaxed more slowly. However, as was the case for npq2, the amplitude of the signal was much larger than expected, given the fact that the amount of qE was again less than in the wild type. In contrast, {Delta}A535 in lut2 was much slower to form than in the wild type and had lower amplitude, consistent with the smaller qE. Hence, discrepancy between the amplitude of {Delta}A535 and the amount of qE was only found in the two mutants that had deepoxidation states larger than were formed in the wild type.


Figure 6
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Figure 6. Light-dependent kinetics of qE-related {Delta}A535 conformational changes at 700 µmol photons m–2 s–1 and qE absorption difference spectra of wild-type and xanthophyll mutant leaves dark adapted for 30 min. A and B, Kinetics of {Delta}A535, with traces as labeled. Six to 10 kinetic traces were averaged (error ± 5%). C and D, qE absorption difference spectra (5 min of light minus 5 min of dark relaxation) for the wild type (WT; solid line), npq2 (short dashed line), npq1 (long dashed line), lut2 (dashed dotted line), lut2npq2 (medium dashed line), and lut2npq1 (dotted line).

 
The absorption difference spectra of the qE-related conformational changes were recorded in the xanthophyll mutants in order to provide clues about which xanthophylls were involved (Fig. 6, C and D). The difference spectrum for npq1 was nearly identical to that of the wild type (Fig. 6C), with negative bands at 438, 468, and 495 nm. The positive band was shifted to around 525 nm, as found in DTT-treated wild-type leaves (Fig. 4C). Consistent with the much reduced qE in this mutant, the amplitudes of all bands were much less than those found in the wild-type spectrum. The difference spectrum of npq2 showed some differences from the wild type. The amplitude of the positive 535-nm band was the same as in the wild type but was slightly red shifted to around 537 nm. In contrast, the negative bands in this spectrum were all of lower amplitude than in the spectrum for the wild type, with a slight broadening and a red shift of the 495-nm band. The negative and positive bands in the lut2 difference spectrum were all of smaller amplitude than in the wild-type spectrum, consistent with the reduced qE in this mutant (Fig. 6D). The 495-nm negative band was again red shifted slightly to around 497 nm. In the difference spectrum of the lut2npq2 mutant, the amplitude of the 535-nm band was enhanced relative to the band in the lut2 mutant, consistent with the {Delta}A535 data. As in npq2, the wavelength maximum was red shifted to around 537 nm. Interestingly, however, the negative bands were smaller and there was a strong red shift of the 495-nm band to around 501 nm. The complete absence of either the negative or the positive band in the lut2npq1 difference spectrum demonstrated that all of the features of the spectrum are entirely related to qE (Fig. 6D) and that the electrochromic shift ({Delta}A = 518 nm) makes negligible contribution to the steady-state spectra, as found previously (Li et al., 2000Go). The transient qE generated at low light intensity was also found to be associated with a transient increase in 535-nm absorption. The light-minus-recovery spectrum of this transient absorption change was virtually identical to the steady-state spectrum observed at high light intensity (Supplemental Fig. S2).


    DISCUSSION
 TOP
 ABSTRACT
 RESULTS
 DISCUSSION
 MATERIALS AND METHODS
 LITERATURE CITED
 
We have tested the hypothesis that zeaxanthin-dependent and zeaxanthin-independent components of NPQ arise from two separate mechanisms (type I and type II, respectively), occurring in different parts of the LHCII/PSII complexes. Contrary to the predictions of this hypothesis, it was found that both NPQ components shared a similar sensitivity to changes in the protein compositions of both the minor monomeric and the major trimeric LHCII antenna. Thus, the amplitudes of both NPQ components were reduced in kolhcb6, aslhcb4, and aslhcb2 plants compared with wild-type plants. The observation that the zeaxanthin-dependent NPQ was reduced in these plants is consistent with the fact that xanthophyll cycle pigments are bound to the minor monomeric antenna and trimeric LHCII (Ruban et al., 1999Go, 2002aGo) and with the previously documented effects of these xanthophylls on quenching of all of these complexes in vitro (Ruban et al., 1996Go, 1997Go; Wentworth et al., 2000Go). The data also suggest that qE is unlikely to arise solely in the minor monomeric antenna proteins of PSII, as proposed many times (Gilmore et al., 1998Go; Ahn et al., 2008Go). These conclusions are consistent with the finding that, while no individual Lhcb protein appears to be obligatory for qE, each one may play a role in shaping the PSII macrostructure for the optimal combination of light harvesting and photoprotection (Horton et al., 2008Go) and with studies on the chlorophyll b-less mutants with severely reduced PSII antenna size that showed strong reductions in NPQ capacity (Härtel et al., 1996Go; Gilmore et al., 2000Go). The disruptive effect of the depletion of Lhcb proteins on the PSII macrostructure is well documented (Horton et al., 2008Go). Indeed, even in aslhcb2 plants, in which the lateral C2S2M2 arrangement of PSII is maintained (Ruban et al., 2003Go), the replacement of Lhcb1 and -2 by Lhcb5 leads to weaker grana stacking forces (E.-H. Kim, W.S. Chow, and J.M. Anderson, unpublished data). Thus, the proper arrangement of PSII and grana stacking appears to be essential for fully functional NPQ. Additional insight into the structural basis of NPQ has been obtained in this investigation by analysis of the in vivo absorption change at {Delta}A535, which arises from the conformational changes within the PSII antenna that accompany the formation of the quenched state (Ruban et al., 1993bGo; Bilger and Björkman, 1994Go). As found for the PSII macrostructure, {Delta}A535 was sensitive to the loss of both minor monomeric and trimeric LHCII proteins. Again, {Delta}A535 was correlated with both the zeaxanthin-dependent and zeaxanthin-independent components of qE, the shift to shorter wavelength in the latter reflecting the involvement of xanthophylls in this change.

Deficiencies in Lhcb proteins affected not only the amplitude of NPQ but also the kinetics of formation and relaxation. The rate of relaxation of NPQ was faster in the absence of Lhcb6 and slower in the absence of Lhcb1 and -2. In neither case was there evidence of two components to the relaxation kinetics that may have arisen if zeaxanthin-dependent and zeaxanthin-independent quenching were caused by different type I and type II mechanisms and/or within different complexes. In dark-adapted leaves, the differences in the formation kinetics of the zeaxanthin-dependent qE arise at least in part from the altered kinetics of deepoxidation. In kolhcb6, the rate of deepoxidation was accelerated compared with the wild type, while in aslhcb2, it was retarded. The reasons for the differences in deepoxidation kinetics are unclear at present, but we suggest that they are also a consequence of the altered macrostructure and antenna protein composition.

The differences in kinetics of zeaxanthin-dependent quenching cannot be fully explained by altered deepoxidation rates. Thus, the plots of the rates of violaxanthin deepoxidation against the rate of development of the zeaxanthin-dependent component of NPQ were not the same in the mutants and the wild type (i.e. the sensitivity to zeaxanthin was variable). Thus, while aslhcb4 had a similar sensitivity to zeaxanthin as the wild type, aslhcb2 was less sensitive and kolhcb6 was more sensitive. Reduced sensitivity of qE to the {Delta}pH in aslhcb2 was recently described (Pérez-Bueno et al., 2008Go), indicating that there is a generally dampened response in this mutant: less sensitive to zeaxanthin and {Delta}pH; slow kinetics of qE formation and relaxation; and a slow rate of deepoxidation. In contrast, in the absence of Lhcb6, qE appears more responsive: fast rates of formation and relaxation of qE; increased rate of deepoxidation; and increased sensitivity to zeaxanthin, although the maximal amplitude is reduced, probably because of reduced sensitivity of qE to {Delta}pH (Pérez-Bueno et al., 2008Go). It is suggested, therefore, that the alterations in PSII macrostructure influence the dynamics of the conformational changes that underlie the formation of the quenched state.

Investigation of mutants deficient in specific xanthophylls confirmed the conclusions that arose from the study of the Lhcb mutants. As argued above, if type I and type II mechanisms both contribute to qE, there would be discrete kinetic components from each mechanism. In contrast to this prediction, only one component of qE relaxation was observed, the rate of which was regulated by the level of zeaxanthin. In the type I mechanism, zeaxanthin is the quencher and its level would not affect the relaxation kinetics. In contrast, the role of zeaxanthin as an allosteric regulator, proposed in the type II mechanism, readily explains the changes in relaxation kinetics. The effect of zeaxanthin in slowing qE relaxation has been reported previously (Noctor et al., 1991Go). Here, it was found that the relaxation of qE in npq1 was faster than in the wild type, whereas in npq2 and lut2npq2, qE relaxation was significantly retarded.

Measurement of fluorescence lifetimes confirmed the suggestion that the extra zeaxanthin in npq2 and lut2npq2 caused a prequenching of Fm (Dall'Osto et al., 2005Go; Kalituho et al., 2006bGo). In these mutants, all of the violaxanthin, including that bound to the L2 site in the minor antenna complexes, is replaced by zeaxanthin. Indeed, a slight quenching in reconstituted minor antenna complexes having a similar xanthophyll composition to that of these mutants has been observed (Crimi et al., 2001Go; Dall'Osto et al., 2005Go). However, it is important to note that no additional capacity for NPQ is conferred by the presence of extra zeaxanthin. In fact, the lifetime measurements confirm that in lut2npq2, NPQ capacity is significantly reduced.

The perturbation of the capacity and kinetics of NPQ formation in lutein-deficient mutants, observed previously and repeated here, lends some support for the presence of a type II mechanism. Both zeaxanthin-dependent and zeaxanthin-independent qE were affected, the latter being almost completely eliminated. However, the presence of zeaxanthin-dependent qE in the absence of lutein, albeit kinetically different in the mutants compared with the wild type, indicated the lack of an obligatory requirement for lutein. It is clear that when either zeaxanthin or violaxanthin replaces lutein in the internal binding sites in Lhcb proteins, quenching still occurs, but both the dynamics and amplitude of qE are affected. These data, therefore, add to previous work demonstrating the importance of lutein for fully functional qE (Pogson et al., 1998Go; Pogson and Rissler, 2000Go). We suggest that it is the reported structural destabilization of PSII antenna proteins in the absence of lutein (Lokstein et al., 2002Go; Havaux et al., 2004Go), at the level of individual monomers, that undermines the conformational changes leading to formation of the quenched state.

Exploration of the absorption changes associated with qE formation gave some insight into how the xanthophyll composition perturbed the conformational changes. The constitutive presence of zeaxanthin in npq2 and lut2npq2 increased the amplitude of the {Delta}A535 signal, consistent with its identification by Raman spectroscopy as the origin of the 535-nm band (Ruban et al., 2002bGo). Most significant is the observation that in lut2npq2, the increase in {Delta}A535 was accompanied by a reduction in amplitude of qE. Thus, in all other mutants (both xanthophyll and Lhcb mutants) in the presence and absence of DTT, there was a linear correlation between the amplitudes of {Delta}A535 and qE (Fig. 7A ). The broken correlation between {Delta}A535 and qE in lut2npq2 suggests that the absorption change does not directly reflect the formation of a quenching species, consistent with a recent report (Kalituho et al., 2006aGo). A similar conclusion can be drawn from the appearance of the large transient in {Delta}A535 in the kolhcb6 mutant that was not associated with a similar transient in NPQ. Therefore, it is suggested that {Delta}A535 monitors the structural change associated with amplification of qE by zeaxanthin. Indeed, one possible explanation of the origin of the red-shifted zeaxanthin accounting for {Delta}A535 is the formation of a dimer (Ruban et al., 1993aGo; Bonente et al., 2008Go) between a molecule bound at the LHCII V1 site and one bound to a neighboring complex. In the absence of zeaxanthin, the position of the band maximum shifted to around 525 nm, as found previously in isolated chloroplasts (Noctor et al., 1993Go). At present, it is not possible to assign this band to another particular xanthophyll. The slight red shift observed in npq2 and lut2npq2, in which the V1 site is 100% filled by zeaxanthin, suggests that {Delta}A535 may be composed of a mixture of bands from 525 to 540 nm, representing different xanthophyll occupancies of the V1 site depending upon the deepoxidation state.


Figure 7
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Figure 7. Relationship between qE amplitude and qE-related absorption changes in wild-type (WT) , Lhcb, and xanthophyll mutant leaves. A, {Delta}A535 versus qE. The deviation of lut2npq2 from the linear relationship is highlighted with a circle. B, {Delta}A495 versus qE. Data were obtained as in Figures 1, 3, 5, and 6.

 
Improved resolution of the negative bands (495, 468, and 438 nm) in the qE-related absorption difference spectra provides an indication of the complexity of the changes in pigment configurations upon the establishment of qE. Consistent with this finding, light-minus-recovery Raman difference spectra of leaves and chloroplasts show loss of resonance below 500 nm, while it is gained above 500 nm, reflecting exactly the same negative and positive features of the qE absorption difference spectra (Ruban et al., 2002bGo). The position of the 495-nm band was red shifted when lutein was replaced by zeaxanthin or violaxanthin in lut2npq2 and lut2 mutants, consistent with the assignment of this band to lutein (Ruban et al., 2000Go). In contrast to the behavior of the 535-nm band, the amplitudes of these bands were reduced in lut2npq2 compared with the wild type, therefore being better correlated with qE (Fig. 7B). Thus, it is suggested that this observation provides support for the involvement of the L1 domain in qE, as in the type II mechanism.

Analysis of the 535-nm absorption change also suggested that the qE that is transiently formed at low light intensity also involves conformational changes within the PSII antenna. Previously, qE formed under these conditions was ascribed to quenching in the PSII reaction center (Finazzi et al., 2004Go), but here it was shown to be accompanied by an absorption change with the same spectrum as that associated with steady-state qE formed in high light. It was also shown that the transient qE was affected by alteration in the xanthophyll composition in the same way as steady-state qE, adding to previous results (Kalituho et al., 2007Go); thus, the transient qE was strongly reduced in lut2 and lut2npq2 and completely absent in the lut2npq1 mutant. When combined with the reported dependence of transient qE upon PsbS (Finazzi et al., 2004Go; Kalituho et al., 2007Go), these data strongly suggest that it originates from the same common PSII antenna-based mechanism as steady-state qE in high light.

In summary, the evidence that both the zeaxanthin-independent and zeaxanthin-dependent components of qE arise from the same mechanism within the PSII antenna has been strengthened. Both are enhanced by PsbS overexpression (Li et al., 2002Go; Crouchman et al., 2006Go), and both preferentially quench LHCII fluorescence emission bands (Ruban et al., 1991Go). Both components of qE are reduced in amplitude in the absence of lutein (Pogson et al., 1998Go; Niyogi et al., 2001Go). Now, it has been demonstrated that both were affected by changes in the minor monomeric and trimeric LHCII protein composition and both were accompanied by conformational changes leading to very similar absorption changes in the Soret region. Despite different Lhcb protein and xanthophyll compositions, qE was found to consistently relax as a single component even though the half-times differed by greater than 15-fold. All of these findings are consistent with a type II mechanism involving the xanthophyll at the L1 binding site, which is activated by the LHCII conformational change that leads to neoxanthin distortion (Ruban et al., 2007Go) and is allosterically regulated by deepoxidation state at the V1 site (Horton et al., 2005Go). This may take place in some or all of the Lhcb-containing antenna complexes (Ruban et al., 1996Go; Mozzo et al., 2008Go). The alternative possibility is that a type I mechanism occurs in both trimeric LHCII and the minor monomeric antenna and that, in the absence of zeaxanthin, a lutein cation can take its place as the quencher. However, irrespective of which mechanism is involved, it is abundantly clear from the data presented here that the natural xanthophyll composition and Lhcb protein content within the PSII antenna is necessary for a fully functional NPQ, in which the conformational dynamics are tuned to create maximum flexibility between efficient light harvesting in low light and rapid formation and relaxation of photoprotection in fluctuating light.


    MATERIALS AND METHODS
 TOP
 ABSTRACT
 RESULTS
 DISCUSSION
 MATERIALS AND METHODS
 LITERATURE CITED
 

Plants and Growth Conditions

Arabidopsis (Arabidopsis thaliana ‘Columbia’) and mutant and transgenic lines derived from it were grown for 8 to 9 weeks in Sanyo plant growth cabinets with an 8-h photoperiod at a light intensity of 100 µmol photons m–2 s–1 and day/night temperatures of 22°C/15°C. The xanthophyll mutants used were as follows: npq1 (mutated in violaxanthin deepoxidase and therefore unable to synthesize zeaxanthin in excess light); npq2 (mutated in zeaxanthin epoxidase and constitutively containing zeaxanthin even in low light, while lacking violaxanthin and neoxanthin; Niyogi et al., 1998Go); lut2 (lacking the expression of functional lycopene {varepsilon}-cyclase and lacking lutein; Pérez-Bueno and Horton, 2008Go); lut2npq2 (possessing zeaxanthin as the only xanthophyll; Havaux et al., 2004Go); and lut2npq1 (lacking lutein and unable to deepoxidate violaxanthin to zeaxanthin; Niyogi et al., 2001Go). The Lhcb protein mutants used were as follows: aslhcb2 (lacking Lhcb1 and -2; Andersson et al., 2003Go); kolhcb6 (mutated in Lhcb6; Kovacs et al., 2006Go); and aslhcb4 (Andersson et al., 2001Go). For the latter mutants, as = antisense and ko = T-DNA knockout.


Chlorophyll Fluorescence Induction

Chlorophyll fluorescence was measured with a Dual PAM 100 chlorophyll fluorescence photosynthesis analyzer (Heinz Walz). The plants were adapted in the dark for 30 min prior to measurement. Actinic illumination (700 µmol photons m–2 s–1) was provided by arrays of 635-nm light-emitting diodes illuminating both the adaxial and abaxial surfaces of the leaf. Fo (the fluorescence level with PSII reaction centers open) was measured in the presence of a measuring beam of 10 µmol photons m–2 s–1. The maximum fluorescence in the dark-adapted state (Fm), during the course of actinic illumination (Fm'), and in the subsequent dark relaxation periods was determined using a 0.8-s saturating light pulse (4,000 µmol photons m–2 s–1). The quantum yield of PSII (Fv/Fm) was defined as (Fm Fo)/Fm, and NPQ was defined as (FmFm')/Fm'. The reversible component of NPQ (relaxing within 5 min) was assigned to energy-dependent NPQ (qE) and calculated as (Fm/Fm') – (Fm/Fm''), where Fm'' is the maximal yield of fluorescence after 5 min of dark relaxation following the actinic illumination. Leaves were vacuum infiltrated with a 5 mM DTT solution in order to completely inhibit violaxanthin deepoxidation. Analysis of the kinetics of NPQ was carried out using a SigmaPlot software curve-fitting procedure (SPSS).


Chlorophyll Fluorescence Lifetimes

Time-correlated single photon counting measurements were performed using a FluoTime 200 picosecond fluorometer (PicoQuant). Detached leaves were vacuum infiltrated with 50 µM nigericin to completely inhibit NPQ. Excitation at a 10-MHz repetition rate was provided by a 470-nm laser diode, which was carefully adjusted to completely close all PSII reaction centers without causing photoinhibitory quenching of Fm and to be far below the onset of singlet-singlet exciton annihilation. For measurement of Fm' values, NPQ was induced at 700 µmol photons m–2 s–1 by arrays of 635-nm light-emitting diodes illuminating both the adaxial and abaxial surfaces of the leaf. Fluorescence was detected at 685 nm with 2-nm slit width. The instrumental response function was in the range of 50 ps. For lifetime analysis, FluoFit software (PicoQuant) was used.


Absorption Changes in Whole Leaves

Absorption changes in the 410- to 565-nm region were measured using a SLM DW2000 dual-wavelength spectrophotometer. Whole Arabidopsis leaves were detached from plants dark adapted for 30 min, and the petioles were wrapped in moist filter paper. The actinic light (700 µmol photons m–2 s–1) illuminated the leaf at 45° and was defined using a Corning 5-58 filter. The photomultiplier was protected using a Corning 4-96 filter and an OCLl Cyan T400-570 mirror. The instrument slit width was 5 nm, and the scan rate was 2 nm s–1. {Delta}A535 and {Delta}A505 kinetics were recorded using the wavelength pairs 535 to 565 nm and 505 to 565 nm, respectively. The sample compartment was water cooled to maintain the leaf temperature at 22°C. The kinetics and spectra were normalized upon the chlorophyll a maximum at 435 nm to account for slight differences in chlorophyll content between the mutants.


Pigment Analysis

Pigment composition was determined by reverse-phase HPLC using a LiChrospher 100 RP-18 column (Merck) and a Dionex Summit chromatography system as described previously (Johnson et al., 2008Go). Pigments were extracted from 1-cm2 leaf discs frozen immediately either after 30 min of dark adaptation or after two illumination cycles as described above.


Supplemental Data

The following materials are available in the online version of this article.

Supplemental Figure S1. Kinetics of transient NPQ at 100 µmol photons m–2 s–1 in wild-type and xanthophyll mutant leaves.
Supplemental Figure S2. Kinetics of {Delta}A535 conformational changes and qE absorption difference spectra at 100 µmol photons m–2 s–1 measured in wild-type leaves.


    ACKNOWLEDGMENTS
 
We thank Patrick Romano for assistance isolating the SALK T-DNA knockout of lut2, Stefan Jansson and Jakob Damkjaer for providing seeds of aslhcb4, aslhcb2, and kolhcb6, and Kris Niyogi for providing seeds of lut2npq1 and lut2npq2 mutants.

Received September 16, 2008; accepted November 11, 2008; published November 14, 2008.


    FOOTNOTES
 
1 This work was supported by grants to A.V.R. and P.H. from the Biotechnology and Biological Sciences Research Council and by the Intro2 Marie Curie Research Training Network of the European Union. Back

The author responsible for distribution of materials integral to the findings presented in this article in accordance with the policy described in the Instructions for Authors (www.plantphysiol.org) is: Alexander V. Ruban (a.ruban{at}qmul.ac.uk).

[W] The online version of this article contains Web-only data. Back

www.plantphysiol.org/cgi/doi/10.1104/pp.108.129957

* Corresponding author; e-mail a.ruban{at}qmul.ac.uk.


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