Tree Physiology 28, 761–771 © 2008 Heron Publishing—Victoria, Canada Leaf physiological versus morphological acclimation to high-light exposure at different stages of foliar development in oak J. RODRÍGUEZ-CALCERRADA,1 P. B. REICH,2 E. ROSENQVIST,3 J. A. PARDOS,1 F. J. CANO1 and I. ARANDA4,5 1 Unidad de Anatomía, Fisiología y Genética Forestal, Escuela Técnica Superior de Ingenieros de Montes, Universidad Politécnica de Madrid (UPM), Ciudad Universitaria s/n, E-28040, Madrid, Spain 2 Department of Forest Resources, University of Minnesota, St. Paul, MN 55108, USA 3 Department of Agricultural Science, University of Copenhagen, Hojbakkegaard Allé 21, DK-2630 Taastrup, Denmark 4 Centro Nacional de Investigación Forestal (CIFOR), Instituto Nacional de Investigación Agraria y Alimentaria (INIA), Apdo. 8111, E-28080, Madrid, Spain 5 Corresponding author ([email protected]) Received June 18, 2007; accepted September 18, 2007; published online March 3, 2008 Summary We investigated light acclimation in seedlings of the temperate oak Quercus petraea (Matt.) Liebl. and the co-occurring sub-Mediterranean oak Quercus pyrenaica Willd. Seedlings were raised in a greenhouse for 1 year in either 70 (HL) or 5.3% (LL) of ambient irradiance of full sunlight, and, in the following year, subsets of the LL-grown seedlings were transferred to HL either before leaf flushing (LL-HLBF plants) or after full leaf expansion (LL-HLAF plants). Gas exchange, chlorophyll a fluorescence, nitrogen fractions in photosynthetic components and leaf anatomy were examined in leaves of all seedlings 5 months after plants were moved from LL to HL. Differences between species in the acclimation of LL-grown plants to HL were minor. For LL-grown plants in HL, area-based photosynthetic capacity, maximum rate of carboxylation, maximum rate of electron transport and the effective photochemical quantum yield of photosystem II were comparable to those for plants grown solely in HL. A rapid change in nitrogen distribution among photosynthetic components was observed in LL-HLAF plants, which had the highest photosynthetic nitrogen-use efficiency. Increases in mesophyll thickness and dry mass per unit area governed leaf acclimation in LL-HLBF plants, which tended to have less nitrogen in photosynthetic components and a lower assimilation potential per unit of leaf mass or nitrogen than LL-HLAF plants. The data indicate that the phenological state of seedlings modified the acclimatory response of leaf attributes to increased irradiance. Morphological adaptation of leaves of LL-HLBF plants enhanced photosynthetic capacity per unit leaf area, but not per unit leaf dry mass, whereas substantial redistribution of nitrogen among photosynthetic components in leaves of LL-HLAF plants enhanced both mass- and area-based photosynthetic capacity. Keywords: competitive ability, nitrogen partitioning, photosynthetic acclimation, Quercus petraea, Quercus pyrenaica. Introduction Plants regulate photosynthetic processes in response to changes in irradiance that occur on various time scales (Külheim et al. 2002, Schurr et al. 2006). For example, the onset of mechanisms of thermal dissipation in the light-harvesting complexes, as well as the engagement of alternative non-photosynthetic electron pathways, can protect the photosynthetic apparatus from oxidative damage after shaded plants are exposed to a sudden increase in irradiance (Ort 2001). However, the ability of preexistent foliage to acclimate to changes in light environment requires a transition from high light-use efficiency under low irradiances to high photosynthetic capacity under high irradiances (Hikosaka and Terashima 1995). Such a transformation enhances total carbon assimilation and reduces susceptibility to photoinhibition (Baker and Oxborough 2004). Nitrogen availability, allocation and remobilization (e.g., increasing uptake by roots, or translocation among plant organs or photosynthetic components) play a role in acclimation to a changed light environment (Naidu and DeLucia 1997a, Ramalho et al. 2000, Frak et al. 2001, Walters 2005). The ratio of leaf chlorophyll to nitrogen (e.g., Ellsworth and Reich 1992), Rubisco, cytochrome f or the electron transport rate decrease with an increase in irradiance (Yin and Johnson 2000, Walters 2005), suggesting a reallocation of nitrogen from light-harvesting to energy-transformation processses and the balancing of antenna size relative to photosystem content. Studies of leaf nitrogen fractionation (i.e., among light-harvesting pigments, electron transport chain proteins, carbon fixation enzymes and non-photosynthetic components) show rapid modulation following a change in light environment (Frak et al. 2001). In contrast, anatomical features of shadedeveloped leaves do not change as readily (Eschrich et al. 1989, Sims and Pearcy 1992), limiting complete acclimation of photosynthesis to the light environment in some instances 762 RODRÍGUEZ-CALCERRADA ET AL. (Tognetti et al. 1998, Oguchi et al. 2003, 2005). The rate and extent of photosynthetic acclimation to increased irradiance differ among species with contrasting adaptive strategies. For example, drought-adaptive traits may constrain acclimation of photosynthesis to increasing irradiance (cf. Valladares et al. 2000), whereas shade-adaptation may involve traits that limit light processing at high irradiances (Seemann et al. 1987, Strauss-Debenedetti and Bazzaz 1991). Here, we studied light acclimation in foliage of sympatric and closely related oak species, the temperate Quercus petraea (Matt.) Liebl. and the sub-Mediterranean marcescent Quercus pyrenaica Willd., which coexist in scattered stands throughout central and midwestern Spain, where Q. petraea is at the southern extreme of its distribution. The acclimatory responses of these seedlings to light may help account for differences in their recruitment patterns in the Mediterranean (Gómez-Aparicio et al. 2006). We hypothesized that, during long-term acclimation to increased irradiance, there are physiological changes reflected in leaf nitrogen fractionation, and leaf morphological changes, particularly in the structure of mesophyll tissue. We postulated that acclimatory responses to increased irradiance depend on species and when during leaf development the change in light environment occurs. (and LL-HLBF and LL-HLAF) plants, at a leaf temperature of 25.8 ± 0.1 °C, and over a broad range of intercellular CO2 concentrations (Ci ) generated by increasing the CO2 supply in twelve steps from 50 to 1800 ppm. After 30 min at saturating light and 380 ppm of CO2, the CO2 concentration was reduced step-wise to minimum values, then increased to 380 ppm CO2 again, and lastly increased to high values. Photosynthetic capacity on a leaf area basis (Amax,a) was estimated as the mean of the three measurements made at 1800 ppm and saturating light. A nonlinear least squares fitting procedure was performed to estimate the maximum rates of carboxylation (Vcmax,a) and electron transport (Jmax,a ) from the An –Ci curves. Regression models were constructed according to equations of Farquhar et al. (1980), in which An is modeled as the minimum of Rubisco-limited (Ac) or RuBP-limited (Aj ) photosynthetic rate: An = min( Ac , Aj ) − Rd A c = V cmax , a Aj = J Materials and methods Experimental design and treatments In spring 2004, Q. petraea and Q. pyrenaica seeds from a mixed forest at the southern extreme of the distribution of Q. petraea (41°7′ N, 3°30′ W) were sown in plastic pots (400-cm3 in volume, 35-cm deep) filled with a 3:1 (v/v) peat and sand mixture supplemented with slow-release fertilizer (5 g dm – 3 ). Germinated seedlings were raised in a greenhouse either without shading except by the greenhouse structure (HL, 70% of full midday ambient photosynthetic photon flux (PPF) on a sunny day = 1050 ± 28 µmol m – 2 s –1 ), or beneath a shade cloth (LL, 5.3% of full midday ambient PPF on a sunny day = 80 ± 7 µmol m – 2 s –1 ). At the end of the growing season, seedlings were transplanted individually to cylindrical PVC containers (3000 cm3, 40 cm deep), in the same medium newly supplemented with slow-release fertilizer. Night–day ranges in temperature and relative humidity were 15–39 °C and 50–90%, respectively. All seedlings were well watered during the experiment. The next year, six plants per species were moved from LL to HL either 1 week before leaf flushing (February 27; LLHLBF) or after full leaf expansion (June 6, 3 months after leaf emergence; LL-HLAF). First-flush leaves from LL, LLHLBF, LL-HLAF and HL plants were measured, or harvested for measurement on July 3–7. Photosynthesis was measured the week ending May 30. Gas exchange measurements Net CO2 assimilation rate (An ) was measured with an infrared gas analyzer (LC pro Analytical Development, U.K.) in a PPF of 1000 µmol m – 2 s –1 for HL and 700 µmol m – 2 s –1 for LL Ci − Γ* 1+ O C i + Kc Ko Ci − Γ* O 4 C i + τ (1) (2) (3) where Rd is mitochondrial respiration rate, which was estimated from Ac. The concentration of oxygen (O) was considered to be 20 kPa. Temperature-dependent parameters Kc (Michaelis-Menten constant of Rubisco for CO2 ) and Ko (Michaelis-Menten constant of Rubisco for O2 ) were calculated for the leaf temperature of each curve following the equations derived by Bernacchi et al. (2001); temperature dependency of the CO2 specificity factor (τ) was accounted for by the equation derived by Harley et al. (1992). The CO2 compensation point in the absence of mitochondrial respiration in light (Γ* ) was calculated as O/ 2τ. The light dependence of the rate of electron transport (J ) was calculated as: J= αQ αQ 1+ Jmax, a (4) 2 where α is the efficiency of light utilization (0.24 mol e – (mol quanta) – 1 ) and Q is the incident photon flux. All parameters were entered for modeling functions. Estimates of Vcmax,a and Jmax,a at 25 °C were obtained by rearranging the temperature-dependent equations of Vcmax,a and Jmax,a given by Dreyer et al. (2001) for Q. petraea. Mass-based estimates (Amax,m, Vcmax,m and Jmax,m ) were obtained by dividing area-based values by leaf dry mass per unit area (MA ). Nitrogen concentration and fractioning among leaf proteins Values of Vcmax,a and Jmax,a at 25 °C were used to calculate leaf TREE PHYSIOLOGY VOLUME 28, 2008 LEAF RESPONSES TO LIGHT IN TWO CO-OCCURRING WHITE OAKS nitrogen fractions in Rubisco (Pr) and in photosynthetic electron transport proteins (Pb ), respectively, following equations in Niinemets and Tenhunen (1997): Pr = Pb = V cmax, a (5) 6.25 Vcr M A Nm Jmax, a rescence signal approached steady-state (Fs ) in actinic light, a similar flash was applied to obtain a value of the maximum fluorescence in light (Fm′). The minimum fluorescence in light (Fo′) was measured at each PPF by applying a 5-s far-red light pulse in temporary darkness to drain electrons from the electron acceptors of PSII. The redox state of the primary electron acceptor QA of PSII (qL ) was calculated according to Kramer et al. (2004): (6) 8.06 Jmc M A Nm –1 where the value 6.25 g Rubisco (g N in Rubisco) converts nitrogen concentration to Rubisco protein concentration, the value 8.06 µmol cytochrome f (g N in bioenergetics) – 1 is a conversion factor based on the assumption that there is a constant 1:1:1.2 cytochrome f:ferredoxin NADP reductase:coupling factor stoichiometry controlling electron transport, Vcr is specific activity of Rubisco at 25 °C (20.5 µmol CO2 (g Rubisco) – 1 s –1 ) and Jmc is the capacity of electron transport per unit of cytochrome f at 25 °C (156 mol e– (mol cytochrome f) – 1 s – 1 ). Leaf nitrogen concentration per unit dry mass (Nm ) was measured, excluding petioles, by the Kjeldahl procedure (Bradstreet 1965). We used MA to express nitrogen concentration on an area basis (Na = Nm MA ). Values of leaf chlorophyll concentration per unit dry mass (Cm ) (determined following Barnes et al. 1992) were used to calculate the fractions of chlorophyll associated with photosystem (PS) I, PSII and light harvesting complex II. Previously, we calculated the concentration of these protein complexes on a leaf area basis according to equations in Hikosaka and Terashima (1995) and Niinemets and Tenhunen (1997). The proportion of nitrogen in light-harvesting components (Pl ) was computed as: Pl = 763 Cm (7) Nm C B where CB is the weighted average of chlorophyll binding of the three protein complexes (see Hikosaka and Terashima 1995). The proportion of structural nitrogen was calculated as Ps = 100 – Pl – Pr – Pb. Photosynthetic nitrogen-use efficiency (PNUE) was estimated as Amax,m /Nm. Chlorophyll fluorescence measurements Light response curves of chlorophyll fluorescence parameters were measured with a portable pulse-modulated fluorometer (FMS 2, Hansatech Instruments, Norfolk, U.K.) to examine PSII acclimation. Attached leaves of five plants per treatment of Q. petraea and Q. pyrenaica were alternately measured between 1100 and 1400 h over 3 days. Measurements were made in a growth chamber with leaf temperature kept around 25 °C by setting the air temperature to 23.5 °C and relative humidity to 65%. For the two highest PPFs, a fan was used to prevent leaf temperature from rising above 28 °C. Leaves were darkened for 20 min before measurements to obtain minimum (Fo ) and maximum (Fm ) values of fluorescence by applying a 0.8-s saturating pulse (PPF = 6600 µmol m – 2 s –1 ). When the fluo- qL = Fm ′ − Fs Fo ′ Fm ′ − Fo ′ Fs (8) The yield of the three competing pathways of de-excitation of chlorophyll in PSII, i.e., the yields of photochemistry of PSII (ΦPSII), down-regulatory non-photochemical quenching (ΦNPQ ) and other energy losses (ΦNO ) were also calculated (Kramer et al. 2004): Φ PSII = Fm ′ − Fs (9) Fm ′ Φ NPQ = 1 − Φ PSII − Φ NO Φ ΝΟ = 1 Fm ′ NPQ + 1 + q L Fo − 1 (10) (11) where NPQ is non-photochemical quenching of absorbed energy at each PPF: NPQ = Fm − Fm ′ Fm ′ (12) The rate of electron transport through PSII (ETR) was calculated following Rosenqvist and van Kooten (2003): ETR = 0. 5Φ PSII PPF 0.84 (13) Nonlinear regression models were fitted to describe the variations in photochemical and non-photochemical yields with PPF for each seedling. The light response of ETR was modeled by a single exponential function (Rascher et al. 2000) to estimate the maximum electron transport rate (JETR ). Steadystate was estimated from the Fs value, rather than from Fm′, which requires more time to reach a true steady state. The curves thus resemble rapid light response curves where the apparent rate of electron transport is slightly underestimated (White and Critchley 1999). The presence of the experimenter in the growth chamber increased the CO2 concentration from 380 to 550 ppm. Hence, we could not assess mesophyll conductance from combined gas exchange and chlorophyll fluorescence measurements. TREE PHYSIOLOGY ONLINE at http://heronpublishing.com 764 RODRÍGUEZ-CALCERRADA ET AL. Anatomical variables Sections of leaf blades held in fresh carrot pith were cut around the middle region and immersed in formalin:acetic acid:ethanol (FAA; 5:5:90, v/v) for 24 h. The FAA was then replaced by 70% ethanol until analysis. Measurements were made, with a light microscope, on sections taken halfway between the mid-rib and the edge. The cell content was destroyed with sodium hypochlorite and further stained to better distinguish tissues. The thicknesses of adaxial plus abaxial epidermis, palisade parenchyma, spongy parenchyma and leaf lamina were measured at three locations on five leaves per species per light treatment. Statistical analysis Most variables were transformed to meet assumptions of parametric analysis. We performed two-way analyses of variance (ANOVA) to test for the significance of light treatment and species on each variable. To test the hypothesis that acclimation differs between species, we included the interaction term between light treatment and species in the variance model. We used Tukey’s Honestly Significant Difference (HSD) test to explore differences (at P < 0.05) between treatments. Results Gas exchange parameters Parameters expressed on an area basis were higher in HL plants than in LL plants. For both species, Amax,a increased on exposure to high light in LL-HLAF and LL-HLBF plants to values slightly lower than, but not significantly different from, values in HL plants, and significantly higher (50%) than values in LL plants. Values of Jmax,a and Vcmax,a increased on exposure to high light in LL-HLBF and LL-HLAF plants compared with LL plants (Table 1). On a mass basis, Amax,m, Vcmax,m and Jmax,m did not differ between LL and HL plants. Among treatments, Amax,m was higher in LL-HLAF plants, but it did not differ significantly among LL, HL and LL-HLBF plants. Both Vcmax,m and Jmax,m were higher in LL-HLAF plants than in LL-HLBF plants and were generally at intermediate values in LL and HL plants (Table 1). There were clear differences between species irrespective of light treatment, but both species responded similarly to the treatments. Quercus petraea had higher Amax,m, Vcmax,m and Jmax,m than Q. pyrenaica, but there were no differences when the variables were expressed on an area basis (Table 1). There was no effect of species or light treatment on Jmax /Vcmax. Mesophyll resistances to CO2 diffusion, ignored in this study, would have lowered estimates of Vcmax, but would have barely affected Jmax, resulting in the large Jmax /Vcmax ratios observed across treatments (Piel et al. 2002). Chlorophyll fluorescence parameters In both species, JETR and qL were higher in HL plants than in LL plants (Table 2). Values of JETR and qL were similar in LL-HLAF and LL-HLBF plants, but significantly higher than in LL plants and lower than, but not significantly different from, values in HL plants (Table 2). The relative contributions of photochemical (ΦPSII) and down-regulatory non-photochemical (ΦNPQ ) mechanisms for processing absorbed light were similar among LL-HLBF, LL-HLAF and HL plants, and different from those of LL plants (Table 2, Figure 1). In LL plants, ΦPSII was lower and ΦNPQ higher than in plants in the other treatments. Accordingly, the PPF at which ΦNPQ was greater than ΦPSII was lowest in LL plants (about 225 µmol m – 2 s – 1 ) and higher (about 700 µmol m – 2 s – 1 ) in LL-HLBF, LL-HLAF and HL plants of Q. pyrenaica, and the corresponding values for Q. petraea ranged from about 350 µmol m – 2 s – 1 in LL plants to about 500 –550 µmol m – 2 s – 1 in LL-HLBF, LL-HLAF and HL plants (Figure 1). The pattern of ΦNO did not vary between species or among light treatments. Quercus pyrenaica seedlings had higher JETR and ΦPSII(1100) than Q. petraea seedings. Between LL-HLAF and LL plants, ΦNPQ(1100) and the curvature of the light-response curves of ΦPSII and ΦNPQ (parameter b of the nonlinear regression models; Figure 1) were similar in Q. petraea but differed in Q. pyrenaica (Table 1; Pinteraction (Pint ) < 0.05 considering only the LL and LL-HLAF treatments). Biochemical parameters Mass-based leaf nitrogen concentration was lower in HL and LL-HLBF plants than in LL plants, whereas it was intermediate in LL-HLAF plants. In contrast, Na was similar and higher in HL and LL-HLBF plants than in plants in the other treatments (Table 3). The LL plants had a higher Pl than the HL and LL-HLAF plants, with LL-HLBF plants having intermediate values. Values of Pb were slightly higher in HL plants than in LL plants, LL-HLAF plants had the highest values, and values in LL-HLBF plants were closer to LL values than to HL values. Light treatment had a weak effect on Pr (P = 0.048), being higher in LL-HLAF plants than in LL-HLBF plants and similar in LL and HL plants. There was no significant effect of light treatment on Ps ; however, there was a tendency for a higher Ps in LL-HLBF plants. When nitrogen fractions were calculated per unit of photosynthetic nitrogen, LL and LLHLBF plants had less nitrogen in Rubisco [Pr /(Pr + Pb + Pl )] than LL-HLAF and HL plants, and nitrogen in bioenergetics [Pb /(Pr + Pb + Pl )] was similar and higher in HL, LL-HLBF and LL-HLAF plants than in LL plants (data not shown). Photosynthetic nitrogen-use efficiency was highest in LLHLAF plants, and intermediate in HL plants and similar in both species. Both Nm and Pl were significantly higher in Q. petraea than in Q. pyrenaica, independent of light treatment, whereas the reverse was true for Na and Ps. There was a clear tendency for seedlings having a greater fraction of nitrogen in photosynthetic components to have a higher photosynthetic capacity (Figure 2). In both species, Amax,m was positively correlated with both Pr and Pb (Figures 2a and 2b). As a result, there was a negative relationship between Amax,m and Ps (Figure 2d). No significant relationship was observed between Amax,m and Pl or Nm (Figures 2c and 2e). Similar results were obtained with Vcmax,m and Jmax,m, in place of Amax,m (data not shown). There were weak positive correlations between MA and Ps (r 2 = 0.19, P < 0.1 for Q. pyrenaica and r 2 = 0.26, P < 0.05 for Q. petraea). TREE PHYSIOLOGY VOLUME 28, 2008 LEAF RESPONSES TO LIGHT IN TWO CO-OCCURRING WHITE OAKS 765 Table 1. Means (± SE) of gas exchange parameters (n = 4–5), and F values and their significance (denoted by asterisks: * = P < 0.05; ** = P < 0.01; and *** = P < 0.001) from two-way ANOVAs. Different letters indicate significantly different treatment means at P < 0.05 (Tukey’s HSD test following ANOVA), for both species combined when Pint = 0.05. Abbreviations: LL, plants in low light; LL-HLBF, LL plants transferred to high light before leaf flushing; LL-HLAF, LL plants transferred to high light after leaf flushing; HL, plants in high light; Amax,a and Amax,m, photosynthetic capacities per unit area (µmol m – 2 s –1 ) and per unit mass (µmol g – 1 s – 1 ), respectively; Vcmax,a and Vcmax,m maximum rates of carboxylation per unit area (µmol m – 2 s –1 ) and per unit mass (µmol g – 1 s – 1 ), respectively; Jmax,a and Jmax,m maximum rates of electron transport per unit area (µmol m – 2 s –1 ) and per unit mass (µmol g – 1 s – 1 ), respectively; and Jmax /Vcmax, ratio of maximum electron transport to maximum carboxylation. Treatment Amax,a Amax,m Vcmax,a Vcmax,m Jmax,a Jmax,m Jmax /Vcmax Quercus pyrenaica LL 20.5 ± 1.5 a LL-HLBF 33.9 ± 2.7 b LL-HLAF 36.2 ± 2.2 b HL 41.9 ± 5.0 b 0.50 ± 0.04 a 0.46 ± 0.04 a 0.73 ± 0.06 b 0.61 ± 0.11 a 54.0 ± 4.4 a 70.8 ± 5.8 ab 72.9 ± 8.5 b 77.2 ± 4.8 b 1.32 ± 0.08 ab 0.97 ± 0.08 a 1.47 ± 0.20 b 1.12 ± 0.13 ab 87 ± 9 a 144 ± 12 b 156 ± 14 b 183 ± 22 b 2.14 ± 0.22 a 1.96 ± 0.14 a 3.15 ± 0.36 b 2.68 ± 0.49 ab 1.63 ± 0.15 2.04 ± 0.16 2.19 ± 0.14 2.37 ± 0.21 Quercus petraea LL 24.8 ± 1.5 a LL-HLBF 34.1 ± 2.0 b LL-HLAF 34.8 ± 2.3 b HL 35.4 ± 1.3 b 0.68 ± 0.06 a 0.59 ± 0.04 a 0.85 ± 0.03 b 0.60 ± 0.04 a 57.9 ± 3.9 a 70.5 ± 1.2 ab 76.9 ± 9.7 b 86.3 ± 10.6 b 1.58 ± 0.12 ab 1.22 ± 0.06 a 1.89 ± 0.23 b 1.48 ± 0.22 ab 106 ± 5 a 149 ± 9 b 151 ± 13 b 158 ± 11 b 2.89 ± 0.21 a 2.57 ± 0.18 a 3.70 ± 0.20 b 2.71 ± 0.26 ab 1.86 ± 0.16 2.11 ± 0.14 2.01 ± 0.14 1.87 ± 0.13 F value Treatment Species Interaction 8.94*** 7.01* 0.91 5.35** 0.70 0.08 5.52** 9.77** 0.08 11.93*** 0.04 1.01 7.24** 8.54** 0.73 2.66 0.75 2.03 14.66*** 0.21 1.47 Morphological and anatomical parameters As expected, MA was lower in LL plants than in HL plants. For transferred plants, leaves that developed in high light (LL-HLBF) had similar MA as HL plants, with MA being intermediate in LL-HLAF plants (Table 4). Across all light treat- ments, MA was higher in Q. pyrenaica than in Q. petraea. Lamina thickness changed with light treatment mainly because of changes in the palisade parenchyma (Table 4, Figure 3). Leaves of HL and LL-HLBF plants were thicker and had thicker palisade parenchyma (generally with two layers of Table 2. Means (± SE) of chlorophyll fluorescence parameters (n = 4–5), and F values and their significance (denoted by asterisks: * = P < 0.05; ** = P < 0.01; and *** = P < 0.001) from two-way ANOVAs. Different letters indicate significantly different treatment means at P < 0.05 (Tukey’s HSD test following ANOVA), for both species combined when Pint = 0.05. Abbreviations: LL, plants in low light; LL-HLBF, LL plants transferred to high light before leaf flushing; LL-HLAF, LL plants transferred to high light after leaf flushing; HL, plants in high light; JETR (µmol m – 2 s – 1 ), maximum electron transport rate from fluorescence; qL(1100), photochemical quenching at 1100 µmol m – 2 s – 1 PPF; ΦPSII(1100), effective photochemical quantum yield of PSII at 1100 µmol m – 2 s –1 PPF; ΦNPQ(1100), yield of downregulatory non-photochemical quenching at 1100 µmol m – 2 s –1 PPF; bΦPSII and bΦNPQ, curvature of light responses of ΦPSII and ΦNPQ, respectively. Treatment JETR qL(1100) ΦPSII(1100) ΦNPQ(1100) bΦPSII (10 –3 ) bΦNPQ (10 –3 ) Quercus pyrenaica LL LL-HLBF LL-HLAF HL 53 ± 9 a 123 ± 12 b 123 ± 12 b 140 ± 16 b 0.13 ± 0.02 a 0.25 ± 0.03 b 0.23 ± 0.02 b 0.27 ± 0.03 b 0.12 ± 0.01 a 0.26 ± 0.02 b 0.26 ± 0.02 b 0.29 ± 0.03 b 0.63 ± 0.01 b 0.50 ± 0.04 a 0.50 ± 0.02 ab 0.50 ± 0.04 a 4.30 ± 0.60 b 1.74 ± 0.17 a 1.47 ± 0.14 a 1.57 ± 0.17 a 4.11 ± 0.56 b 1.29 ± 0.15 a 1.12 ± 0.17 a 1.35 ± 0.22 a Quercus petraea LL LL-HLBF LL-HLAF HL 61 ± 6 a 93 ± 16 b 93 ± 13 b 107 ± 20 b 0.12 ± 0.01 a 0.19 ± 0.03 b 0.23 ± 0.03 b 0.25 ± 0.06 b 0.13 ± 0.01 a 0.20 ± 0.03 b 0.20 ± 0.03 b 0.23 ± 0.04 b 0.59 ± 0.02 b 0.55 ± 0.03 a 0.58 ± 0.03 ab 0.53 ± 0.02 a 2.89 ± 0.51 b 2.26 ± 0.45 a 2.41 ± 0.55 a 1.84 ± 0.56 a 2.69 ± 0.52 b 1.74 ± 0.35 a 2.08 ± 0.51 a 1.70 ± 0.61 a F value Treatment Species Interaction 8.38*** 4.74* 0.95 6.40** 1.13 0.39 9.31** 4.38* 0.94 4.61** 2.27 1.65 9.02*** 1.09 1.58 7.38** 0.49 2.70 TREE PHYSIOLOGY ONLINE at http://heronpublishing.com 766 RODRÍGUEZ-CALCERRADA ET AL. Figure 1. Photochemical and non-photochemical yields of absorbed energy with photosynthetic photon flux (PPF) [ΦPSII = m + aexp(–bPPF); ΦNPQ = m(1 – exp(–bPPF)); ΦNO = m – aexp(–bPPF)] in seedlings of Quercus pyrenaica and Q. petraea. Treatments: (a, b) low light; (c, d) plants transferred to high light 1 week before leaf flushing; (e, f ) plants transferred to high light 3 months after leaf flushing; and (g, h) high light. Symbols: ΦPSII, 䉱 and 䉭; ΦNPQ, 䊏 and 䊐; and ΦNO, 䊉 and 䊊. Vertical lines indicate PPF at which ΦPSII = ΦNPQ. Values are means (n = 4–5) ± SE. palisade cells) than LL and LL-HLAF plants, with some differences between species in these patterns (Pint < 0.05). Quercus pyrenaica seedlings generally had thicker palisade parenchyma in the HL treatment and thinner palisade parenchyma in the LL treatment than Q. petraea seedlings. Leaves of LLHLAF plants barely altered their anatomy on exposure to high light, although two out of the five samples of Q. pyrenaica (none of Q. petraea) had a double layer of palisade cells, resulting in a slight increase in lamina thickness compared with LL samples, which had a single layer of palisade cells. There were no significant effects of light or species on the thickness of epidermal and spongy parenchyma tissues. Therefore, the ratio of palisade to spongy parenchyma thickness was similar and higher in LL-HLBF (1.63) and HL (1.46) plants compared with LL (0.67) and LL-HLAF (0.87) plants (Pspecies > 0.15, Pint > 0.15). Discussion Leaf plasticity to light in long-term acclimated plants Quercus petraea and Q. pyrenaica leaves acclimated both functionally and structurally to the prevailing irradiance. The HL plants had thicker leaves, with a thicker palisade parenchyma, and greater Vcmax, Jmax and Amax,a than the LL plants (cf. Ellsworth and Reich 1992, Evans and Poorter 2001). Such changes enabled HL plants to exploit high irradiances more efficiently than LL plants, because they can regenerate more NADP and ADP to alleviate the over-reduction of PSII centers at high PPFs and minimize the risk of photoinhibition (Chow 1994, Baker and Oxborough 2004). This functional difference would partly explain the gentler decline in ΦPSII with increasing PPF in HL plants compared with LL plants (Figure 1), although differences in the rate of photosynthetic induction between LL and HL plants cannot be ignored. Some acclimatory changes in the fractionation of nitrogen among pools increased photosynthetic capacity in HL plants (Hikosaka and Terashima 1995, Niinemets and Tenhunen 1997, Niinemets et al. 1998). Values of Pr were similar among treatments, although Pb tended to be higher in HL than in LL plants at the expense of lower Pl (Table 3). Nitrogen fractions in Rubisco and bioenergetics expressed per unit of photosynthetic nitrogen were also higher in HL plants than in LL plants. TREE PHYSIOLOGY VOLUME 28, 2008 LEAF RESPONSES TO LIGHT IN TWO CO-OCCURRING WHITE OAKS 767 Table 3. Means (± SE) of biochemical parameters (n = 4–5), and F values and their significance (denoted by asterisks: * = P < 0.05; ** = P < 0.01; and *** = P < 0.001) from two-way ANOVAs. Different letters indicate significantly different treatment means at P < 0.05 (Tukey's HSD test following ANOVA), for both species combined when Pint = 0.05. Abbreviations: LL, plants in low light; LL-HLBF, plants transferred to high light before leaf flushing; LL-HLAF, plants transferred to high light after leaf flushing; HL, plants in high light; Nm (mg g – 1 ), nitrogen concentration per unit leaf mass; Na (g m – 2 ), nitrogen concentration per unit leaf area; Pl (%), nitrogen fraction in light-harvesting components; Pb (%), nitrogen fraction in electron transport proteins; Pr (%), nitrogen fraction in Rubisco; Ps (%), nitrogen fraction in structural components; and PNUE (µmol g –1 s –1 ), photosynthetic nitrogen-use efficiency. Treatment Nm Na Pl Quercus pyrenaica LL 29.9 ± 1.8 b LL-HLBF 27.5 ± 1.4 a LL-HLAF 28.8 ± 1.0 ab HL 26.9 ± 0.9 a 1.23 ± 0.10 a 1.99 ± 0.10 b 1.44 ± 0.07 a 1.93 ± 0.11 b 24.9 ± 2.5 b 19.9 ± 2.8 ab 18.5 ± 1.4 a 18.2 ± 1.7 a 5.7 ± 0.4 a 5.8 ± 0.6 a 8.8 ± 1.1 b 7.7 ± 1.3 b 34.4 ± 0.9 ab 28.2 ± 3.5 a 39.9 ± 5.5 b 31.8 ± 3.8 ab 35.0 ± 2.9 46.0 ± 6.2 32.8 ± 7.4 42.4 ± 5.7 16.9 ± 1.4 a 17.1 ± 1.3 a 25.3 ± 2.2 b 22.1 ± 3.5 ab Quercus petraea LL 35.1 ± 1.8 b LL-HLBF 28.5 ± 1.8 a LL-HLAF 32.2 ± 1.8 ab HL 27.2 ± 1.8 a 1.29 ± 0.05 a 1.61 ± 0.11 b 1.33 ± 0.15 a 1.61 ± 0.11 b 30.7 ± 1.2 b 23.9 ± 2.3 ab 25.2 ± 2.7 a 20.3 ± 1.8 a 6.5 ± 0.3 a 7.1 ± 0.4 a 9.2 ± 0.4 b 8.0 ± 0.8 b 35.2 ± 3.2 ab 33.5 ± 2.6 a 45.7 ± 4.4 b 42.9 ± 6.5 ab 27.6 ± 4.4 35.4 ± 3.2 19.9 ± 5.6 28.8 ± 7.8 19.2 ± 1.2 a 20.6 ± 1.4 a 26.8 ± 1.5 b 22.4 ± 1.7 ab F value Treatment Species Interaction 12.51*** 4.97* 1.48 5.27** 9.15** 0.42 7.12*** 3.32 0.33 2.93* 3.60 0.46 2.32 7.24* 0.11 7.71*** 1.92 0.24 6.43** 6.58* 1.16 Pb Pr Ps PNUE Figure 2. Relationships between leaf nitrogen estimated in (a) Rubisco (Pr ), (b) photosynthetic electron transport (Pb ), (c) light harvesting (Pl ) and (d) structural components (Ps ), and (e) mass-based leaf nitrogen concentration (Nm ), with mass-based photosynthesis in seedlings of Q. petraea (open symbols, dashed lines) and Q. pyrenaica (filled symbols, continuous lines) treated with low light (䊊, 䊉), high light (䊐, 䊏), plants transferred to high light 1 week before leaf flushing (䉭, 䉱) and plants transferred to high light 3 months after leaf flushing (䉫, 䉬) . Regression lines are (a): y = 0.45 lnx – 0.73 for Q. pyrenaica and y = 0.28 lnx – 0.17 for Q. petraea, (b): y = 0.49 lnx – 0.25 for Q. pyrenaica and y = 0.57 lnx – 0.36 for Q. petraea, (d): y = –0.49 lnx + 2.58 for Q. pyrenaica and y = –0.36 lnx + 2.07 for Q. petraea; regression lines indicated when P < 0.1. TREE PHYSIOLOGY ONLINE at http://heronpublishing.com 768 RODRÍGUEZ-CALCERRADA ET AL. Table 4. Means (± SE) of morphological parameters (n = 4–5), and F values and their significance (denoted by asterisks: * = P < 0.05; ** = P < 0.01; and *** = P < 0.001) from two-way ANOVAs. Different letters indicate significantly different treatment means at P < 0.05 (Tukey’s HSD test following ANOVA), for both species combined when Pint = 0.05. Abbreviations: LL, plants in low light; LL-HLBF, LL plants transferred to high light before leaf flushing; LL-HLAF, LL plants transferred to high light after leaf flushing; HL, plants in high light; MA (g m – 2 ), leaf dry mass per area; TL (µm), leaf thickness; TE (µm), epidermis thickness; TPP (µm), palisade parenchyma thickness; and TSP (µm), spongy parenchyma thickness. Treatment MA TL TE TPP TSP Quercus pyrenaica LL LL-HLBF LL-HLAF HL 40.9 ± 1.0 c 72.6 ± 1.5 a 50.3 ± 2.2 b 67.9 ± 3.7 a 91 ± 3 a 132 ± 8 bc 112 ± 6 ab 154 ± 13 c 24.2 ± 1.3 28.3 ± 1.3 27.0 ± 0.9 28.5 ± 2.5 26.3 ± 1.0 a 59.1 ± 6.2 bc 41.7 ± 5.7 ab 75.1 ± 7.0 c 40.3 ± 2.0 44.4 ± 3.3 43.2 ± 1.4 50.0 ± 4.3 Quercus petraea LL LL-HLBF LL-HLAF HL 37.4 ± 1.4 c 56.6 ± 2.2 a 40.9 ± 2.9 b 58.7 ± 2.5 a 101 ± 4 a 134 ± 7 b 99 ± 3 a 128 ± 4 b 25.0 ± 0.9 27.4 ± 1.2 25.9 ± 1.5 26.4 ± 0.7 30.5 ± 1.1 a 69.5 ± 5.6 b 30.9 ± 1.9 a 59.1 ± 2.9 b 45.3 ± 2.3 37.5 ± 3.6 41.7 ± 1.2 42.1 ± 2.3 F value Treatment Species Interaction 62.04*** 29.64*** 1.07 22.73*** 1.21 2.89* 1.91 0.61 0.37 52.70*** 0.87 3.57* 1.02 2.38 2.42 Light-induced increases in MA (i.e., increased mesophyll tissue) are sometimes more important in enhancing photosynthetic capacity than variations in nitrogen allocation within leaves (Ellsworth and Reich 1992, Evans and Poorter 2001, Parelle et al. 2006, Katahata et al. 2007), as is supported by our finding of a constant amount of photosynthetic machinery per unit dry mass in LL and HL seedlings of both species (i.e., similar values of Vcmax,m, Jmax,m and Amax,m; Table 1). Hence, Q. petraea and Q. pyrenaica seedlings acclimated to the prevailing irradiance, but did so in slightly different ways. Quercus petraea seedlings had greater plasticity in leaf nitrogen concentration and partitioning to light-harvesting pigments, whereas Q. pyrenaica seedlings had greater plasticity in mesophyll thickness, chlorophyll fluorescence parameters and area-based gas exchange parameters. These results are consistent with the slightly superior shade tolerance of Q. petraea (Rodríguez-Calcerrada et al. 2007a, 2007b) as discussed elsewhere (Niinemets 1997, Cao 2000, Niinemets and Valladares 2004). ditional layer, thereby increasing the proportion of HLadapted palisade chloroplasts relative to chloroplasts in the spongy mesophyll (Terashima and Inoue 1984). Thus, leaf acclimation to HL is governed by the accumulation of photosynthetic tissue per unit area. Area-based photosynthetic parameters of LL-HLBF leaves increased as much as in LL-HLAF leaves, and did not differ significantly from those of HL leaves. In contrast, mass-based estimates (Vcmax,m, Jmax,m and Amax,m ) in LL-HLBF leaves were similar or slightly lower than in LL and HL leaves, but lower than in LL-HLAF leaves (Table 1). Nitrogen redistribution among photosynthetic components on transfer from LL to HL would have contributed to reduced photosynthetic efficiency per unit dry mass in LLHLBF plants. A higher MA in LL-HLBF leaves is likely due to a greater mesophyll cell wall thickness, which would explain the tendency for a greater quantity of structural nitrogen components in these leaves, which might limit CO2 diffusion into the chloroplasts (Miyazawa and Terashima 2001) and reduce PNUE (Table 3). Acclimation of leaves of shade-developed plants to high light before flushing High-light acclimation in shade-developed leaves Leaf dry mass per unit area of LL-HLBF leaves increased to HL values 5 months after transfer to the HL treatment, corresponding at least in part to an increase in thickness of the palisade parenchyma (Table 4). Others have reported significant increases in lamina thickness in tree species of various successional positions and shade-tolerances when irradiance increased before bud break (Goulet and Bellefleur 1986, Aranda et al. 2001), indicating considerable anatomical flexibility in shade-induced primordia (cf. Eschrich et al. 1989). It is likely that, in LL-HLBF leaves, palisade parenchyma cells enlarged while developing in high light and then divided to form an ad- Leaves of both oak species acclimated to HL after flushing in LL, as observed in both evergreen and deciduous trees (Strauss-Debenedetti and Bazzaz 1991, Naidu and DeLucia 1997b, 1998). Oguchi et al. (2003) reported that a limited capacity for change in thickness of mature shade-developed leaves limits photosynthetic acclimation to increased irradiance. In our study, however, after only 4 weeks of HL exposure, and despite little anatomical change, Amax,a, Vcmax,a, Jmax,a and PNUE all increased in leaves of LL-grown plants transferred to HL. On a dry mass basis, key photosynthetic traits, Vcmax,m and Jmax,m , increased rapidly following transfer from LL to HL (Tables 1–3). We suggest that rapid reorganization TREE PHYSIOLOGY VOLUME 28, 2008 LEAF RESPONSES TO LIGHT IN TWO CO-OCCURRING WHITE OAKS 769 Figure 3. Transverse sections of leaves of seedlings of Q. pyrenaica (a–d) and Q. petraea (e–h). Depth of sections is 20–30 µm. Treatments: (a, e) high light; (b, f) plants transferred to high light 1 week before leaf flushing; (c, g) plants transferred to high light 3 months after leaf flushing; and (d, h) high light. Bars respresent 50 µm. in the protein pool largely accounted for this pattern (Yamashita et al. 2000, Frak et al. 2001, Han et al. 2006) and counteracted the carry-over effects of anatomical shade acclimation of the LL-grown plants. On exposure to HL, Pl decreased in parallel with increased Pr and Pb, suggesting a rapid remobilization of nitrogen among photosynthetic components. The degradation of chlorophyllbinding proteins in response to high irradiances can facilitate the synthesis of Rubisco and compounds involved in electron transport (Yang et al. 1998, Walters 2005). These responses increase photosynthetic light-use efficiency and reduce ΦNPQ (Naidu and DeLucia 1997b, Müller et al. 2001, RodríguezCalcerrada et al. 2007a) by reducing the excess energy to be dissipated (Rosenqvist and van Kooten 2003, Baker and Oxborough 2004; Figure 1, Table 2). Other factors may have contributed to the increased photosynthetic capacity of the LLHLAF plants. For instance, Oguchi et al. (2003 and 2005) found that the surface of chloroplasts facing the intercellular spaces increased after transfer from low to high light as a result of increased chloroplast volume. Interspecific differences in leaf acclimation of shadedeveloped plants We saw differences between species in many leaf traits. Whereas Q. pyrenaica seedlings had a greater capacity for electron transport at high PPF (ΦPSII(1100) and JETR ), Q. petraea seedlings had higher Amax,m, Vcmax,m, Jmax,m and Pl, and lower MA and Ps (Tables 1–4). Lower Amax,m in Q. pyrenaica than in Q. petraea was partly attributable to the greater proportion of non-photosynthetic nitrogen, although differences in photorespiration and internal diffusion of CO2 cannot be ruled out. Additionally, the slower growth of Q. pyrenaica in the month preceding photosynthetic measurements (66% lower height growth than in Q. petraea for all treatments pooled; data not shown) may have caused end-product inhibition of photosynthesis (Paul and Foyer 2001). Overall, these results point to greater shade tolerance and competitive ability of Q. petraea seedlings compared with Q. pyrenaica seedlings (Reich et al. 1999), although PNUE was similar between species (Wright et al. 2001, Lusk et al. 2003). Notwithstanding the poorer photosynthetic perfor- TREE PHYSIOLOGY ONLINE at http://heronpublishing.com 770 RODRÍGUEZ-CALCERRADA ET AL. mance per unit dry mass of Q. pyrenaica seedlings, no differences in the mechanisms of acclimation and negligible differences in the extent of acclimation were observed for a plethora of leaf traits, perhaps because ecological differences between the species are small enough that distinct patterns of acclimation of photosynthesis under conditions of optimal nutrient and water availability do not occur. The only differences in acclimation response between species were in LL-HLAF seedlings, which, in Q. pyrenaica but not Q. petraea, tended to have thicker leaves and palisade parenchyma than LL plants. It is likely that the second layer of palisade cells was already formed before transfer from LL to HL in some Q. pyrenaica seedlings. Significant enlargement of mesophyll cells has been observed in mature leaves of the deciduous species Acer rufinerve Siebold & Zucc. on exposure to high light (Oguchi et al. 2005). In conclusion, leaves of Q. petraea and Q. pyrenaica seedlings acclimated to increased irradiance by an increase in photosynthetic capacity resulting from adjustments in both physiological and morphological traits. The extent of these changes, which were similar in both species, depended on whether the increase in irradiance occurred before or after leaf expansion. Acknowledgments This work was supported by the Consejería de Medio Ambiente y Desarrollo General de la Comunidad Autónoma de Madrid. JR-C was supported by a scholarship from the Consejería de Educación de la Comunidad de Madrid (C.M.) and the Fondo Social Europeo (F.S.E.), and PBR participation was supported in part by the National Science Foundation LTER Program. References Aranda, I., L.F. Bergasa, L. Gil and J.A. Pardos. 2001. 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