Ion antiport accelerates photosynthetic acclimation in fluctuating light environments

Many photosynthetic organisms globally, including crops, forests and algae, must grow in environments where the availability of light energy fluctuates dramatically. How photosynthesis maintains high efficiency despite such fluctuations in its energy source remains poorly understood. Here we show that Arabidopsis thaliana K+ efflux antiporter (KEA3) is critical for high photosynthetic efficiency under fluctuating light. On a shift from dark to low light, or high to low light, kea3 mutants show prolonged dissipation of absorbed light energy as heat. KEA3 localizes to the thylakoid membrane, and allows proton efflux from the thylakoid lumen by proton/potassium antiport. KEA3’s activity accelerates the downregulation of pH-dependent energy dissipation after transitions to low light, leading to faster recovery of high photosystem II quantum efficiency and increased CO2 assimilation. Our results reveal a mechanism that increases the efficiency of photosynthesis under fluctuating light.

E fficient conversion of energy is a critical challenge for all organisms. Energy in the environment is available either as chemical potential or light. Uniquely, the energy available as light can undergo extreme fluctuations in amplitude on short time scales. Photon flux can change 100-fold within seconds, for example, due to shade from clouds or leaves moving in the wind 1,2 . Understanding the mechanisms that underlie efficient photosynthesis in fluctuating light can open doors to increased crop yields, and more broadly can reveal fundamental principles of robust energy conversion systems.
The light reactions of photosynthesis produce NADPH and ATP to power carbon fixation. Light-harvesting antennae absorb photons and transfer their energy to the photosystems, which pump electrons from water to NADPH. This process is coupled to proton translocation across the thylakoid membrane into the thylakoid lumen, which drives ATP synthesis 3,4 . Under high light, the high proton concentration in the thylakoid lumen activates energy-dependent quenching (qE), a mechanism that dissipates absorbed light energy in the PSII antenna as heat 5 . qE is thus part of a negative feedback loop that decreases energy transfer to PSII by up to 75% in response to excess light [6][7][8] .
To maximize yields under continuously changing light intensities, the PSII antenna must rapidly alternate between dissipation of excess absorbed energy under high light, and efficient harvesting of photons for photosynthesis under limiting light 9 . On transition from high to limiting light, the qE energy dissipation mechanism is downregulated to increase the energy available to PSII. However, this downregulation occurs on a timescale of minutes, producing an extended period where heat dissipation of light energy starves the photosystems of excitation energy. Simulations predict that the slow downregulation of heat dissipation mechanisms can reduce the photosynthetic efficiency by B10% in crop canopies 10 . The design principles that determine the kinetics of qE downregulation remain unknown 11 , motivating a search for molecular factors that affect its dynamics.
Here we show that ion antiport activity across the thylakoid membrane accelerates photosynthetic acclimation after a change in light intensity from dark to low light, or from high to low light. In the model plant Arabidopsis thaliana (hereafter 'Arabidopsis'), K þ efflux antiporter 3 (KEA3) is localized in the thylakoid membrane and mediates H þ /K þ antiport. After each transition to low light, KEA3 allows proton efflux from the lumen, which accelerates the downregulation of pH-dependent energy quenching, and transiently increases photosystem II quantum efficiency and CO 2 fixation. Our findings demonstrate that a K þ /H þ antiport activity mediated by KEA3 increases photosynthetic efficiency under fluctuating light conditions.

Results
KEA3 is co-regulated with photosynthesis-related genes. The previously established regulation of qE by thylakoid pH 5 led us to hypothesize that proton/cation antiporters in the thylakoid membrane could regulate the dynamics of qE. We therefore searched for proton/cation antiporters in Arabidopsis that were transcriptionally co-regulated with photosynthesis-related genes. The expression of KEA3 was strongly correlated with genes annotated with the gene ontology (GO) term 'photosynthesis' (Supplementary Fig. 1a, Po10 À 12 , Mann-Whitney U-test). Conversely, the most significantly enriched GO term among the 100 genes whose expression was most highly correlated with KEA3 was 'photosynthesis' (Po10 À 41 ). KEA3 is highly conserved among photosynthetic eukaryotes ( Supplementary  Fig. 1b  encode a predicted chloroplast transit peptide and a cation/H þ antiporter (CPA2) domain (Fig. 1a, Supplementary Fig. 2a). KEA3.2 additionally encodes a carboxyl-terminal (C-terminal) K þ transport/nucleotide-binding (KTN) domain, which is truncated in KEA3.1. Size analyses of the endogenous KEA3 protein and tagged versions of both isoforms indicate that KEA3.2 is the major protein isoform in leaves ( Supplementary Fig. 2). Recently, C-terminal fluorescent protein fusions of KEA3.1 and KEA3.2 were localized to the chloroplast and the Golgi, respectively 12,13 . In contrast to previous work, we observed KEA3.2-green fluorescent protein (GFP) in the chloroplast (Fig. 1b). We confirmed the localization of the endogenous KEA3 to the chloroplast in wild-type (WT) leaves by western blot of total and chloroplast protein extracts (Fig. 1c, Supplementary Fig. 3a). Subfractionation of WT chloroplasts demonstrated that endogenous KEA3 is located in the thylakoid membrane and is enriched in the stromal lamellae (Fig. 1d,e, Supplementary Fig. 3b,c).
KEA3 accelerates photosynthetic acclimation to low light. We analysed the phenotypes of two kea3 mutant alleles, kea3-1 and kea3-2 ( Supplementary Fig. 2). These mutants displayed no measurable defects in growth, leaf colouration or protein composition of the photosynthetic apparatus ( Supplementary Fig. 4). To characterize potential defects in regulation of photosynthesis, we performed chlorophyll fluorescence measurements across various light conditions. We observed a striking perturbation of the kinetics of non-photochemical energy quenching (NPQ) on a shift from dark to low-light conditions. In flowering plants, a shift from a dark-acclimated state to light-limiting conditions causes a transient rise in NPQ, which is attributed to qE 14 . The kea3 mutants displayed a higher maximum NPQ and a delay in its peak and relaxation (Fig. 2a, Supplementary Fig. 5a). This kea3 phenotype was complemented by expressing a KEA3.2-GFP fusion protein that accumulated at levels similar to the native protein ( Fig. 2a, Supplementary Fig. 6). Remarkably, plants overexpressing the amino-terminal part of KEA3 containing the chloroplast transit peptide and CPA2 domains (oeKEA3 CPA2 ) showed accelerated qE relaxation kinetics. When shifted from dark to higher light intensities, kea3 mutants displayed WT-like induction kinetics of NPQ ( Supplementary Fig. 5c,e).
The transient nature of the additional NPQ observed on a shift to low light suggested that qE was perturbed in kea3. qE is known to be modulated by the luminal pH and zeaxanthin, and normal qE kinetics require the protein PsbS 14 . kea3psbs double mutants exhibited the same NPQ kinetics as psbs single mutants (Fig. 2b, Supplementary Fig. 7a), indicating that PsbS is required for the additional NPQ observed in kea3. Double mutants of kea3 with npq1 (lacking zeaxanthin) and npq2 (overaccumulating zeaxanthin) revealed that the NPQ phenotype was modulated by levels of zeaxanthin ( Supplementary Fig. 7b,c). Application of high concentrations of nigericin, which inhibit qE 15 , to leaves, abolished the rapid component of NPQ in both WT and kea3 ( Supplementary Fig. 8a). Thus, the additional NPQ observed in kea3 shows the key characteristics of qE.
The transient increase in NPQ was accompanied by lower PSII quantum yield (F II ) in kea3 (Po0.004, Student's t-test, Fig. 2c), indicating decreased linear electron flow through PSII. This decrease in F II was PsbS dependent ( Supplementary Fig. 7e), suggesting that it was caused by an increase in qE. In oeKEA3 CPA2 , F II was transiently higher than in WT (Fig. 2c). We conclude that KEA3 accelerates qE relaxation, allowing more absorbed light energy to be used to drive electron flow through PSII.
KEA3 likely mediates K þ /H þ antiport. To gain insights into the identity of the cations transported by the CPA2 domain of KEA3, we used phylogenetics. KEA3 shows more sequence homology to experimentally validated K þ /H þ antiporters AtKEA2 (ref. 16) and EcKefC 17 than to Na þ /H þ antiporters EcNhaA and TtNapA (Fig. 3a). Comparison of two amino acid residues critical for Na þ /H þ binding in Na þ /H þ antiporters of the CPA2 family 18,19 indicates that presence of an Aspartate-Aspartate motif strictly correlates with Na þ /H þ antiport activity, while conversion of the first residue to Asparagine or Glutamine correlates with K þ /H þ antiport activity 16,17,20 (Fig. 3b). Like AtKEA2 and EcKefC, KEA3 has a Glutamine-Aspartate motif. Finally, the presence of the K þ transport-related KTN domain in KEA3 further supports a K þ /H þ antiporter activity 21,22 .
We reasoned that if KEA3 is a K þ /H þ antiporter, low concentrations of the small molecule electroneutral K þ /H þ antiporter nigericin might rescue the kea3 phenotype. Strikingly, infiltration of leaves with 0.03 mM nigericin fully rescued the qE phenotype (Fig. 3c, Supplementary Fig. 8a). This result strongly suggests that KEA3 accelerates the qE relaxation by electroneutral K þ /H þ antiport. of the proton motive force (p.m.f.). We performed near-simultaneous measurements of NPQ as a readout of DpH, and of the magnitude of the carotenoid electrochromic shift (ECS t ) 23 as a readout of total p.m.f. (DpH þ Dc), during the transition from dark to low light (Fig. 3d,e). The dynamics of the p.m.f. were largely unchanged in kea3, but the ratio of NPQ to ECS t was higher than in WT, suggesting that KEA3 transiently decreases the contribution of DpH to the proton motive force. We measured both DpH and Dc after 100 s illumination by turning off the light and observing the extended kinetics of the ECS 24 . These measurements indicated that after 100 s of low light, the DpH is greater in kea3 than in WT (Po0.04, Student's t-test, Fig. 3f,g, Supplementary Fig. 8b), consistent with the observed increased NPQ in kea3 at this time point (Figs 2a and 3d, Supplementary Fig. 5a). This difference was not present at higher light intensities. These data further support the idea that KEA3 decreases the contribution of DpH and increases the contribution of Dc to p.m.f.
KEA3 accelerates acclimation from high to low light. Transitions from high to low light are common in many growth environments, including crop canopies 1 . We therefore asked whether KEA3 influences the dynamics of photosynthesis during transitions from high to low light. After a sudden shift from high to low light, NPQ in WT Arabidopsis plants decayed over B80 s   to a new, lower level (Fig. 4a,b, Supplementary Fig. 9a). Strikingly, NPQ decayed more slowly in kea3, while high and low light NPQ values were comparable to WT. The half time of the NPQ decay in kea3 was twice as long as that in WT (Col-0: 24.8 ± 1.4 s, kea3-1: 47.6 ± 3.0 s, P ¼ 4.1 Â 10 À 5 ; Ws: 25.9 ± 1.4 s, kea3-2: 51.8 ± 2.0 s P ¼ 1.8 Â 10 À 6 ( ± s.e.m., Student's t-test)). These data suggest that KEA3 plays a key role in accelerating the decay of NPQ during transitions from excess to limiting light conditions. We observed decreased F II in kea3 (Po0.02, Student's t-test) over a similar time interval to the NPQ defect (Fig. 4c,  Supplementary Fig. 9b). As during transition from dark to low light (Fig. 2a,c), these data suggest that the slower relaxation of NPQ in kea3 results in a transient decrease in linear electron flow relative to WT.
We measured CO 2 assimilation during the same transition. While CO 2 assimilation rates of kea3 and WT plants were similar under steady-state high and low light, kea3 exhibited a period of lower CO 2 assimilation than WT immediately after a transition from high to low light (Fig. 4d,e, Po0.007, Supplementary  Fig. 9c,d, Po0.04). We conclude that following a high-to lowlight transition, KEA3 accelerates the downregulation of qE, thus allowing a larger fraction of the absorbed light energy to drive linear electron flow and CO 2 fixation.

KEA3 improves photosynthetic efficiency in fluctuating light.
To investigate the role of KEA3 under continuously fluctuating light, we exposed plants to alternating cycles of 140 s at high light and 100 s at low light. kea3 mutants consistently showed slower NPQ relaxation and F II recovery than WT after each transition (Fig. 4f,g and Supplementary Fig. 10). These phenotypes were present regardless of whether the fluctuations were preceded by 10 min of high light or 10 min of low light, suggesting that KEA3's function is not extensively affected by preceding light conditions. NPQ and F II in kea3 reached WT levels after the fluctuations stopped, further supporting the role of KEA3 specifically in light transitions. We conclude that KEA3 improves photosynthetic efficiency under continuously fluctuating light.

Discussion
Our data are consistent with the following intriguing model: (i) The dynamics of qE relaxation are dictated by the dynamics of the thylakoid luminal pH. (ii) After a sudden transition to low light, the ATP synthase alone cannot sustain sufficient proton efflux to enable rapid downregulation of qE. (iii) KEA3 overcomes this limitation by providing an additional route for proton efflux, thereby accelerating qE relaxation and increasing photosynthetic yield. KEA3's electroneutral activity would provide two advantages for proton efflux over a simple proton channel: (i) it retains the Dc component of the p.m.f. and (ii) it can rapidly mediate a large flux because its activity does not generate an opposing electric field.
We note that the combined activities of KEA3 and the recently identified thylakoid potassium channel TPK3 (ref. 25 17 . The observation that the kea3 phenotype is specific to transitions to low light suggests that KEA3 might similarly be repressed by NADPH (or alternatively, activated by NADP). KEA3 could thus be a key component of a feedback loop, which detects an oxidized stroma and facilitates reduction of oxidized PSI electron acceptors by downregulating qE. Our work demonstrates that the kinetics of qE decay influence photosynthetic efficiency. Our discovery that plants have a builtin machinery to accelerate these kinetics makes KEA3 a new target for efforts to improve crop productivity. Excitingly, overexpression of the KEA3 CPA2 domain produces a transient increase in the relative CO 2 assimilation rate after transition from high to low light (Supplementary Fig. 9). However, the overexpression of the CPA2 domain appears to also result in undesirable photodamage in high light. It is possible that improved regulation of KEA3 would overcome this limitation. Thus, the future investigation of KEA3 should yield both fascinating insights into the core logic of photosynthesis regulation, as well as keys to possible enhancements in crop yields.

Methods
Plant material, propagation and growth conditions. The kea3-1 mutant (Gabi_170G09) in the Col-0 genetic background originates from the GABI-KAT collection 27 . The kea3-2 mutant (FLAG_493_C01) in the Wassilewskija (Ws) genetic background originates from the FLAGdb/FST T-DNA collection 28 . The aba1 mutant (Salk_059469) in the Col-0 genetic background originates from the SALK T-DNA collection 29 . The npq1 and psbs mutants have been described previously 7 31 . The plants were then transferred to the greenhouse and seeds were collected after 3 weeks. Individual transgenic plants were selected on the basis of their resistance to kanamycin (pJCV55) or Basta (pB7FWG2) on sterile 1% agar media containing 1 Â MS nutrients (PhytoTechnology Laboratories) and 0.05 g l À 01 MES, adjusted to pH 5.7 with KOH. Before transfer to soil, Kanamycin-and Basta-resistant plants were additionally screened for red fluorescent protein and GFP expression, respectively, using an M165 FC fluorescence microscope (Leica) to verify expression of the transgene (the T-DNA deriving from pJCV55 carries an additional red fluorescent protein-encoding gene). The presence of the KEA3 transgene in transformants was confirmed by PCR and its expression was confirmed by protein immunoblot analyses.
WT and mutant Arabidopsis plants were grown on soil under controlled conditions in the greenhouse (matted daylight supplemented with high pressure sodium 400 W lamps, B100 mmol photons m À 2 s À 1 on leaf surfaces, 14/10 h light/dark cycle, constant temperature of 20°C) or in growth chambers (10 h light, 22°C/14 h dark, 23°C, with a light intensity of 100 mmol photons m À 2 s À 1 ).
Nucleic acid analysis. Arabidopsis DNA was extracted using RedExtract-N-Amp (Sigma). T-DNA insertion junction sites were recovered by PCR using combinations of insertion-and gene-specific primers (see Supplementary Table 1), and then sequenced. For reverse transcriptase-PCR (RT-PCR) analysis and cDNA synthesis, RNA was extracted from leaves using the RNeasy plant mini kit (Qiagen) according to the manufacturer's instructions.
The cDNA for cloning purposes was synthesized using Superscript III (Invitrogen). RT-PCR was performed with SuperScript III One-Step RT-PCR System (Invitrogen) and gene-specific primers (see Supplementary Table 1), both according to the manufacturer's instructions.
Fluorescence measurements. Room temperature Chl a fluorescence of whole leaves of 2-3-week-old Arabidopsis plants was measured using an imaging chlorophyll fluorometer (Open FluorCam 800-O/1010; Photon Systems Instruments) or the Dual-PAM 100 (Walz). NPQ during dark-to-light transitions was determined using the FluorCam by acclimating plants for 30 min to dark, followed by 5-10 min at indicated light intensities of red light. To measure Fm and Fm 0 , white light pulses (4,000 mmol photons m À 2 s À 1 , duration 800 ms) were applied. NPQ induction and relaxation during dark to 50, 220 and 660 mmol photons m À 2 s À 1 transitions were monitored using the Dual-PAM by applying red actinic light and white light pulses (4,000 mmol photons m À 2 s À 1 , duration 800 ms) at 20 s intervals. NPQ was calculated as (Fm À Fm 0 )/Fm 0 and F II as (Fm À Fs)/Fm. NPQ relaxation half times were calculated as follows. A steady-state low light average NPQ value was subtracted from the first five data points during the NPQ relaxation period. The binary logarithm of these values was taken, and a linear fitting was performed to obtain a slope s. t 1/2 was calculated as t 1/2 (NPQ) ¼ 1/ À s.
For nigericin rescue experiments, plants were dark adapted for 30 min. Then, leaves were pressed against sand paper to facilitate nigericin uptake and incubated in indicated concentrations of nigericin for 3 h in the dark before measuring NPQ during dark-to-light transitions at 70 mmol photons m À 2 s À 1 .
ECS measurements. Near-simultaneous ECS and fluorescence measurements as well as p.m.f. partitioning analysis were performed on a custom made spectrophotometer/chlorophyll fluorometer chamber with non-focusing optics using three different wavelengths (505, 520 and 535 nm) for deconvoluted ECS measurements 23,32 . Leaves were dark adapted for 30 min before the actinic light of 90 mmol photons m À 2 s À 1 was turned on. Each dark interval relaxation kinetic measurement was made by turning off the actinic light for 200 ms. p.m.f. parsing traces were obtained by turning off the actinic light at 100 s. The ECS steady-state (Dc) and ECS inverse (DpH) were extracted from these traces as described previously 24,33 .
CO 2 assimilation measurements. Plants were grown in 50 ml Falcon tubes with a pierced bottom filled with Sunshine Mix 4 potting mix, placed in a dish containing 1-3 cm of water, under 100 mmol m À 2 s À 1 fluorescent light. For measurement, the Falcon tubes were inserted using a foam gasket into a LI-COR 6400-17 Whole Plant Arabidoposis Chamber. The chamber was placed under a Walz MAXI IMAGING-PAM with blue actinic LEDs, which ran the light programs and was used to simultaneously record chlorophyll fluorescence data. CO 2 assimilation was measured with a reference CO 2 concentration of 400 mmol mol À 1 and a 500 mmol s À 1 flow rate, averaging and recording data over 2 s intervals. The steady-state assimilation rates under high and low light were obtained for each plant by averaging the assimilation rate over the intervals ( À 40 to 0 s) and ( þ 560 to þ 600 s), respectively, and normalizing the assimilation rate by the rosette area measured from IMAGING-PAM images with ImageJ. The transient CO 2 assimilation was calculated as follows. For each plant, the data was normalized so that steady-state high light assimilation rate was 1, and the steady-state low light assimilation rate was 0. The average normalized assimilation rate in each time interval was then calculated for each plant.
Leaf pigment analysis. Pigments were analysed by reverse-phase high-performance liquid chromatography 34 . For pigment extraction, leaf discs were frozen in liquid nitrogen and disrupted with beads in microcentrifuge tubes in the presence of acetone. After a short centrifugation, pigment extracts were filtered through a membrane filter (pore size 0.2 mm) and either used directly for high-performance liquid chromatography analysis or stored for up to 2 days at À 20°C.
KEA3 co-expression analysis was performed by determining Pearson correlation coefficients of all Arabidopsis genes with KEA3 using the GeneCAT database (http://genecat.mpg.de). All genes in the database whose identifiers contained 'At' were used in this analysis. The 100 genes with the highest correlation values were analysed for the enrichment of specific GO terms by using AmiGO (amigo.geneontology.org/cgi-bin/amigo/term_enrichment, 38 ).
Arabidopsis chloroplasts were isolated by a two-step Percoll gradient centrifugation 40 . The homogenized leaf tissue was applied to a two-step Percoll gradient and intact chloroplasts were collected from the interphase. For chloroplast fractionation, chloroplasts were hypotonically lysed in 10 mM Tris/HCl, pH 8.0 and 1 mM EDTA, pH 8.0, at a chlorophyll concentration of 2 mg ml À 1 , and loaded onto a three-step Sucrose gradient 41 . After centrifugation (30,000g; 4°C, 1 h), the upper phase (containing the stroma), the upper interphase (with the envelope membranes) and the pellet (thylakoids) were collected and the proteins were precipitated 42 .
Thylakoid fractionation was performed according to Kyle et al. 43 with minor modifications. Thylakoid membranes at 0.4 mg chlorophyll ml À 1 in 15 mM Tricin/ KOH pH7.8, 0.1 M Sorbitol, 15 mM NaCl, 5 mM MgCl 2 were treated with 0.15% digitonin (w/v) for 1 min and then diluted 10-fold with the same buffer. Samples were then centrifuged at 1,000; 10,000; 40,000; and 150,000g to yield the different fractions.