{'fraction_non_alphanumeric': 0.03162741278554985, 'fraction_numerical': 0.014945989020718966, 'mean_word_length': 5.159685863874346, 'pattern_counts': {'":': 0, '<': 0, '<?xml version=': 0, '>': 0, 'https://': 0, 'lorem ipsum': 0, 'www.': 0, 'xml': 0}, 'pii_count': 0, 'substrings_counts': 0, 'word_list_counts': {'cursed_substrings.json': 1, 'profanity_word_list.json': 0, 'sexual_word_list.json': 0, 'zh_pornsignals.json': 0}}
The rate-limiting step for photosynthetic CO 2 utilization under varying atmospheric evaporative demand in Solanum lycopersicum (tomato)

Background: Despite atmospheric vapour pressure deficit (VPD) was demonstrated as significant environmental factors affecting plant photosynthesis and productivity, the regulating mechanism under varying atmospheric evaporative demand was still unclarified. The contribution of stomatal, mesophyll resistance and biochemical limitation imposed on photosynthesis in tomato under varying evaporative demand was highlighted in the present study. Quantitative photosynthetic limitation analysis across a series of VPD was performed in well-watered tomato, by combining gas exchange and chlorophyll fluorescence. Results: Photosynthetic performance in tomato was gradually depressed with increasing in VPD. Under low VPD condition, stomatal and mesophyll conductance were sufficiently high for CO 2 transport, which facilitated high chloroplast CO 2 concentration for carbon fixation. Stomatal and mesophyll limitation accounted a low fraction, and photosynthetic potential was mostly constrained by biochemical limitation inside chloroplasts under low VPD condition. With increasing in VPD, plant water stress was gradually pronounced and triggered declines in stomatal and mesophyll conductance. Contribution of stomatal and mesophyll limitation on photosynthesis increased gradually with rise in VPD. Consequently, the low CO 2 availability inside chloroplast substantially constrained photosynthesis under high VPD condition. Conclusion: Photosynthetic potential in tomato was mostly constrained by biochemical limitation inside under low VPD condition. CO 2 diffusion limitation in series of and mesophyll resistance was the key rate-limiting step for photosynthesis under high VPD condition.

concentration will rise globally to 550 µmol mol − 1 in the middle of the present century, and increase to 700 ~ 900 µmol mol − 1 by the end of the 21 st century [2,3]. In addition, the greenhouse industry facilitated CO 2 fertilization to enhance plant growth and productivity in the semi-closed ecosystem, which was widely applied throughout the word to improve crop productivity. Although CO 2 fertilization and the globally elevated trends are expected to improve crop photosynthesis and increase yield, large evidence was provided that the magnitude of such enhancement is constrained by other climate change derived phenomena, such as the more extreme and more frequent environmental stress [4].
The bottlenecks constraining CO 2 utilization efficiency is the limited plant photosynthetic capacity for CO 2 acquisition and assimilation.
Photosynthetic CO 2 uptake and transport is constrained by a series of resistance, which was simplified into stomatal and mesophyll resistance [5]. Guard cells of stomata are first "barrier" for gas exchange, which restrict photosynthetic CO 2 uptake and transpiration [6]. In additional to stomatal resistance, large evidences were provided that CO 2 movement from sub-stomatal cavity to carbon fixation site is constrained by the great mesophyll resistance, which substantially depress photosynthesis rate, especially for C 3 plant [7][8][9][10][11][12]. Environmental fluctuation is thought to profoundly affect CO 2 uptake and transport. Large evidences were provided that stomatal and mesophyll conductance respond rapidly and sensitively to the external environmental variation [12][13][14]. It has been recognized that CO 2 movement and carbon fixation is regulated by environmental factors such as soil moisture [15,16], light [17], temperature [18,19] and so on.
Among of these environmental stimulate, effect of atmospheric evaporative demand on photosynthetic CO 2 uptake and transport received far less attention. From a physics perspective, atmospheric vapour pressure deficit (VPD) is evaporative driving force for water transport at leafatmospheric boundary [20]. Previous study demonstrated that VPD regulation profoundly affect plant water status, photosynthetic performance and yield production [21][22][23]. The increasing sophistication of the greenhouse industry facilitates precise atmospheric VPD regulation [24,25]. Despite VPD was 4 an important environmental factor which significantly affect photosynthetic performance, few previous studies have quantitatively addressed the components of photosynthetic limitation under contrasting VPD condition. The rate-limiting step for photosynthetic CO 2 transport and utilization under varying VPD was highly uncertain. A quantitative limitation analysis consisting of stomatal, mesophyll and biochemical limitations was essential to reveal the underlying mechanism of VPD regulating photosynthetic process.
The present study was aimed to identify the rate-limiting process for photosynthetic CO 2 uptake and fixation under varying atmospheric evaporative demand in C 3 plant tomato, by addressing three questions: (1) Which was the most significant limitation for photosynthesis under varying VPD condition.
(2) How did diffusion conductance comparing stomatal and mesophyll conductance tuned with VPD. (3) How did the contribution of stomatal and mesophyll limitation on photosynthesis varied with VPD. In the present study, well-irrigated tomato plants were grown under contrasting VPD condition, in controlled-environment greenhouse.

Effect of VPD on water transport forces along soil-plant-atmospheric continuum
VPD significantly affected the distribution of water free energy along soil-plant-atmospheric pathway, as illustrated in Fig. 1. Atmospheric evaporative demand increased with the rise in VPD, which triggered plant water stress and the linear declines in leaf water potential (Fig. 1A). With rise in VPD, the drawdown of Ψ leaf in high-VPD grown plants was slighter than low-VPD treatment plants, according to the slope of linear regression (Fig. 1A). The driving force for passive water flow between soil and leaf (ΔΨ soil-leaf ) increased with VPD, and the magnitude of increment was greater in low-VPD grown plants than high-VPD plants (Fig. 1B). Since Ψ leaf was negligible compared with the large air negative potential, water driving force at leaf-air boundary (ΔΨ leaf-air ) increased dramatically with rise in VPD, with minor difference among treatments (Fig. 1C). The magnitude for increment in ΔΨ leafair was considerably greater than ΔΨ soil-leaf , and the difference between ΔΨ leaf-air and ΔΨ soil-leaf was enlarged with VPD. The ratio of ΔΨ leaf-air to ΔΨ soil-leaf increased logarithmically from approximately 5 50 at 0.5 KPa to 150 at 1.5 KPa, and then maintained at a steady level (Fig.1D).

Effect of VPD on photosynthetic parameters of tomato
Photosynthesis rate responded to CO 2 elevation in similar patterns regardless of cultivars and growth VPD condition: photosynthesis rate rise rapidly across low CO 2 concentration and then reached a steady-state (Fig.S1). However, the maximum steady-state of photosynthesis rate declined with VPD increased from 0.5 to 4.5 KPa (Fig.S1). Maximum carboxylation rate (V cmax ), maximum electron transport rate (J max ) and carboxylation efficiency (CE) declined linearly with rise in VPD (Fig. 2). The drawdown of V cmax , J max and CE with rise in VPD was moderated in high-grown plants than low-VPD grown plants, according to the slope of linear regression (Fig. 2).

Effect of VPD on photosynthetic CO 2 uptake and transport
Stomatal, mesophyll and total conductance for CO 2 diffusion decreased linearly with increasing VPD, regardless of cultivars and growth VPD condition (Fig. 3). The magnitudes of drawdown in stomatal, mesophyll and total conductance were slighter in high-VPD grown plants than low-VPD grown plants, for both two cultivars (Fig. 3).
The CO 2 concentration of intercellular and chloroplast along the "source-path-sink" was reduced by different extent with rise in VPD (Fig. 4A, B). The drawdowns of C i and C c caused by VPD elevation was relative lower in high-VPD grown plants, compared with low-VPD plants (Fig. 4C, D, E). Consequently, the ratio of C i /C a , C c /C a and C c /C i linearly decreased with rise in VPD. The declining slope of C i /C a , C c /C a and C c /C i versus VPD was lower in high VPD grown plants, compared with low-VPD plants ( Fig.   4C, D, E).

Partial photosynthetic limitation
The fractions of stomatal, mesophyll and biochemical limitation imposed on photosynthesis were not constant, which varied with the rise in VPD (Fig. 5). Under low VPD condition, stomatal and mesophyll conductance for CO 2 diffusion was high and imposed minor limitations on photosynthesis. Stomatal and mesophyll conductance accounted for a low proportion of photosynthetic limitation, while 6 biochemical carboxylation for carbon fixation was the most significant limitation for photosynthetic process under low VPD condition (Fig. 5A, B, C). The fraction of total limitations attributed to stomatal limitation increased linearly with VPD, from approximately 15% at 0.5 KPa to 35% at 4.5 KPa (Fig. 5A).
Similar pattern was observed in mesophyll limitation: The fraction of total limitations attributed to stomatal limitation also increased linearly with VPD, from approximately 23% at 0.5 KPa to 33% at 4.5 KPa (Fig. 5B). The increments in the fractions of stomatal and mesophyll limitation tended to less marked in high VPD grown plants. In contrast, fraction of total limitations attributed to biochemical limitation of carbon fixation gradually linearly decreased with increasing VPD, from approximately 65% at 0.5 KPa to 35% at 4.5KPa (Fig. 5C).
Thereby, biochemical limitation was most significant limitation and rate-limiting step for photosynthetic process under low VPD condition, regardless of cultivars and growth VPD condition ( Fig. 6). The constrains of stomatal and mesophyll limitation imposed on photosynthesis gradually increased and predominated with increasing VPD (Fig. 6). Under high VPD condition, diffusion conductance of stomatal and mesophyll imposed the greatest limitation for photosynthesis in tomato, which were the rate-limiting step for photosynthetic process (Fig. 6).

Correlations among g m , g s , leaf water status and LMA
Leaf mesophyll conductance was significantly and positively correlated with stomatal conductance (Fig. 7A). Meanwhile, stomatal and mesophyll conductance for CO 2 diffusion was closely linked to leaf water status: significant and positive correlations were found in leaf water potential versus stomatal and mesophyll conductance (Fig.7B, C). Acclimation to contrasting VPD condition modified leaf structural traits: LMA tended to be increased in high-VPD grown plants, compared with low-VPD plants ( Fig. S2A). A significant and negative correlation between g m versus LMA was observed (Fig. S2B).

Discussion
The present study demonstrated that photosynthetic performance in tomato was significantly affected by the atmospheric evaporative demand. The proportion of individual limitation components including stomatal conductance, mesophyll conductance and biochemical carboxylation inside chloroplast were not constant with varying VPD. The relative contribution of stomatal, mesophyll 7 resistance and biochemical carboxylation imposed on photosynthesis varied under contrasting VPD condition. Thereby, the key rate-limiting step for photosynthetic performance varied with rise in VPD: under low VPD condition, stomatal and mesophyll conductance was sufficiently high for efficiently CO 2 transport, which facilitated high CO 2 availability inside chloroplast for carbon fixation; diffusion limitation of stomatal and mesophyll conductance accounted for a low fraction of total photosynthetic limitation under low VPD condition, biochemical carboxylation was the key rate-limiting step for raising photosynthetic potential of tomato. With VPD increasing, stomatal and mesophyll conductance for CO 2 transport declined. Stomatal and mesophyll limitation on photosynthesis increased gradually with rise in VPD. Consequently, the low chloroplast CO 2 concentration substantially constrained photosynthesis under high VPD condition. Thereby, CO 2 diffusion limitation in series of stomatal and mesophyll resistance was key rate-limiting step for photosynthesis under high VPD condition.
Three steps were involved in the potential mechanism accounting for the increased significant limitation of stomatal and mesophyll conductance imposed on photosynthesis in tomato with rise in VPD, which was illustrated in Fig.6: (Ⅰ) rise in VPD caused plant water stress via disrupting the mass balance between soil water supply and atmospheric evaporative demand. (Ⅱ) plant water stress with rise in VPD triggered stomatal closure and reduced stomatal conductance for CO 2 uptake. (Ⅲ) leaf anatomical acclimation to atmospheric drought modulated mesophyll conductance for CO 2 transport within leaf.

Rising in VPD triggered plant water stress via disrupting the mass balance between soil water supply and atmospheric evaporative demand
Passive water movement was driven by the gradually declined free energy along soil-plantatmospheric continuum, which can be quantified as the gradient in water potential in liquid phase.
Water movement at leaf-air boundary in gas phase was driven by the difference in VPD. Based on physical principles, excessive air desiccation triggered high VPD and great negative air water potential. Δψ leaf-air was substantial greater than Δψ soil-leaf , which pulled water out of plant. The substantial difference between Δψ leaf-air and Δψ soil-leaf was logarithmically enlarged with rise in VPD. 8 Quantitatively, the atmospheric driving force at leaf-air boundary can be more than a hundredfold larger than soil-leaf component under high VPD condition. The great asymmetric between atmospheric evaporative demand and soil water supply triggered disruption in water balance despite plants were well irrigated. Root water uptake and supply was inadequate to keep pace with the great atmospheric driving force under high VPD condition, which consequently triggered leaf dehydration and declines in water potential. Thereby, VPD was crucial external stimulations pulling water out of soil and affect water balance. VPD fluctuated dramatically over the diurnal course in crop production, especially for greenhouse cultivation. Soil moisture was relatively stable over short term, with a minor variation compared with atmospheric evaporative demand [26]. Plant-water relations was regulated to a greater extent by VPD, and to a less extent modulated by soil moisture. Similar as soil drought, VPD induced atmospheric drought and plant water stress was also important factors triggering depression in photosynthesis.

Plant water stress with rise in VPD triggered stomatal closure and reduced stomatal conductance for CO 2 uptake
Stomata was the "gatekeepers" for exchange of water vapour and CO 2 . Guard cells surrounding the stomatal pore respond to perturbations of soil-plant-atmospheric hydraulic continuum, which was putatively transduced into stomatal movements by feedback and feedforward mechanisms [27][28][29].
Stomatal control of transpired water loss was critical for sustaining physiological processes, such as leaf water status and photosynthetic CO 2 uptake. It has been recognized that plant respond to drought by closing guard cells to reduce excessive water loss and prevent the development of water deficit in plant tissues [30]. In the present study, atmospheric driving force was an order of magnitude greater than water supply, which lead to a great symmetry between water supply and evaporative demand. The water supply-evaporative demand symmetry triggered declines in leaf water potential and stomatal closure. However, the mechanism of VPD-triggered stomatal closure was still uncertain, which was'black box' [31]. Some hypotheses hold that stomatal closure under high VPD condition was a passive process triggered by leaf dehydration and turgor loss. However, large evidences were provided that high-VPD triggered stomatal closure was probably more than a passive process [32].
Some proposed hypothesis hold that high-VPD triggered stomatal closure was an active process rather than passive, since the plant stress hormone of abscisic acid (ABA) was continuously produced and delivered with transpiration stream to guard cell [33,34]. However, it is not clarified whether the ABA mediated active process also participated in VPD-induced stomatal regulation in tomato.
Despite stomatal closure prevented excess water loss to maintain physiological process by passive or active mechanisms, the closed "gatekeepers" simultaneously increased the stomatal resistance for photosynthetic CO 2 uptake from air to intercellular. Intercellular CO 2 concentration was gradually reduced with rise in VPD. Consequently, stomatal limitation imposed on photosynthesis increased with rise in VPD. The declines in leaf water potential and stomatal conductance with rise in VPD was less marked in high-VPD grown plants in this research. The distinct response to VPD may can be attribute to the physiological acclimation to growth condition. Long-term acclimation to high VPD condition enhanced water stress tolerant, which prevent the dramatic declines in leaf water potential, stomatal conductance and photosynthetic parameters when subjected to atmospheric drought.

Anatomical determination for mesophyll conductance of CO 2 transport within leaf under contrasting VPD condition
In additional to the first barrier of stomata, CO 2 transported from intercellular to carboxylation site was constrained by a comparable resistance with stomata. The present study demonstrated that mesophyll resistance was a significant component of diffusion resistance from air to Rubisco in tomato. A strong positive correlation between mesophyll and stomatal conductance was observed among treatments. Similar as stomatal conductance, mesophyll conductance of tomato was also linearly reduced with rise in VPD. Under low VPD condition, stomatal conductance in coupled with mesophyll conductance was sufficiently high for efficient CO 2 transport to carboxylation site within chloroplasts. High diffusion conductance in series of stomatal and mesophyll facilitated high chloroplast CO 2 concentration for carbon fixation. With rise in VPD, CO 2 concentration drawdown along "air-substomatal cavity-chloroplasts" was enlarged. Consequently, CO 2 concentration inside chloroplasts was substantially reduced under high VPD condition. Limitation of mesophyll conductance imposed on photosynthesis gradually dominated with rise in VPD.
Unlike the rapid and sensitive stomatal response to external environment, mesophyll conductance from substomatal cavity to carbon fixation site was determined to a large degree by leaf anatomical traits [35][36][37][38][39]. Leaf dry mass area (LMA) was a composite of underlying traits affecting mesophyll conductance, such as lamina thickness, mesophyll thickness, cell wall thickness, cell shape and bulk leaf density [35]. LMA determined the upper limit on mesophyll conductance. Meanwhile, LMA was closely linked to abiotic stress tolerance [40,41]. Generally, higher LMA was a good indicator of greater stress tolerant. In the present study, LMA of high-VPD grown plants was higher than low-VPD plants. Higher LMA of tomato was an ecological strategy in response to atmospheric drought under high VPD condition. As aforementioned, root water uptake and supply were inadequate to keep pace with the great atmospheric driving force under high VPD condition. A higher LMA indicated dense structural traits, which buffered cellular transpired water loss and prevent leaf tissue dehydration under high VPD condition. However, CO 2 and water transport shared pathway through the mesophyll cell walls and perhaps plasma membranes within leaves [42][43][44][45]. Despite the dense structural traits improved drought tolerance, the resistance for CO 2 diffusion through substomatal cavity to chloroplasts was simultaneously increased. LMA was negatively correlated with mesophyll conductance in the present study, which was consistent with previous studies [46].

Conclusions
Photosynthetic performance of tomato was gradually constrained with rise in atmospheric evaporative demand. The key rate-limiting step for photosynthetic performance varied with rise in VPD. Under low VPD condition, stomatal and mesophyll conductance was sufficiently high and increased CO 2 availability inside chloroplast for carbon fixation; diffusion limitation of stomatal and mesophyll conductance accounted for a low fraction of total photosynthetic limitation under low VPD condition, biochemical carboxylation was the key rate-limiting step for raising photosynthetic potential of tomato. With increasing in VPD, plant water stress was gradually pronounced and triggered linear declines in stomatal and mesophyll conductance. Contribution of stomatal and mesophyll limitation on photosynthesis increased gradually with rise in VPD. Consequently, the low CO 2 availability inside chloroplast substantially constrained photosynthesis under high VPD condition. Thereby, CO 2 diffusion limitation in series of stomatal and mesophyll resistance was the key rate-limiting step for photosynthesis under high VPD condition in tomato.

Plant materials and growth conditions
The experiment was conducted in two controlled-environment greenhouses in same characteristics (15m in length, 10m in width and 3.5m in height, North-South oriented) at Shandong Agriculture University under spring-summer climatic condition, from May to August 2018. Two tomato cultivars [22] (JinPeng NO.1, CV1 hereafter, JinPeng&Co., Ltd., China; FenGuan, CV2 hereafter, ZhongYa &Co., Ltd., China) with distinct VPD response were examined. Seeds were sown in plugs for germination and transplanted at four-leaf stage to 4.5L plastic pots, containing same amount of organic substrate and perlite mixture in a 3:1 proportion (v/v). Soil moisture was maintained around 90% field capacity according to a previous method [21]. Plants were periodically trimmed to maintain rapid vegetative growth throughout experiments. Plants were grown in two environmental-controlled greenhouses, maintained in same growth condition but contrasting VPD: high VPD was achieved in natural greenhouse environment, with VPD approximately 3~5KPa around midday; low VPD was maintained at ranges of 0.5~1.5 KPa by humidification. A high-pressure micro-fog system was activated when VPD exceed the target values, as the characteristics of system were described detailly in a previous study [22].
The effects of VPD perturbations on leaf photosynthetic performance and plant water status were investigated about 50 days after treatments. 15 uniform plants from each treatment were selected as samples and transferred to the growth cabinets in the evening, prior to photosynthetic measurements. Light and temperature of growth cabinets were controlled steadily at normal level throughout the experiment.

Leaf gas exchange and chlorophyll fluorescence
Leaf gas exchange and chlorophyll fluorescence were measured simultaneously on healthy and expanded leaflets at same nodes, by a LI-6400 XT portable gas-exchange system equipped with a leaf chamber fluorometer (LI-6400-40, Li-Cor, Inc., Lincoln, NE, USA). The whole portable gas-exchange system was enclosed in growth cabinets. VPD of growth cabinets and leaf chamber was simultaneously controlled across a series VPD of 0.5, 1.5, 2.5, 3.5 and 4.5KPa. The temperature, light and CO 2 concentration were controlled at a constant and steady condition throughout the experiment: temperature of 30±1℃; a saturating photosynthetic photon flux density (PPFD) of 1000 μmol m -2 s -1 ; CO 2 concentration of 400 μmol mol -1 . VPD was increased stepwise across the gradients for at least 60 min, until photosynthesis and plant water status reached a new steady state.
The curve of photosynthesis rate (P n ) versus intercellular CO 2 concentration (C i ) was performed using a previous procedure [12], under a series VPD of 0.5, 1.5, 2.5, 3.5 and 4.5KPa. Briefly, P n -C i curve was performed by controlling the ambient CO 2 concentration (C a ) from 400 to 300, 200, 150, 100 and 50μmol mol −1 , and then increased to 400μmol mol −1 . After re-achieving a steady-state at 400μmol mol −1 , C a was increased gradually from 400μmol mol −1 to 1200μmol mol −1 . Carboxylation efficiency (CE) was estimated according to linear regression of the P n -C i curve at the ranges of C a ≤ 200μmol mol −1 [47]. The maximum rate Rubisco carboxylation capacity (V cmax ) and maximal rate of electron transport (J max ) were determined according to the FvCB model [48].

Estimation of photosynthetic CO 2 diffusion conductance
A simplified network [12] for CO 2 diffusion via "source-path-sink" was shown in Fig. S3: CO 2 diffusion was constrained by the resistances of stomata and mesophyll in series circuit, driven by the CO 2 partial pressure gradient. CO 2 diffusion conductance through guard cells of stomata (g sc ) was determined according to water diffusion conductance (g sw ), and the ratio between molecular diffusivities of water and CO 2 in gas [49]. Mesophyll conductance (g m ) was estimated by the variable J method [50]:

13
Where P n was the net photosynthesis rate, C i was the intercellular CO 2 concentration. P n and C i was measured by steady-state gas exchange. R d was the mitochondrial respiration rate in the light, and Γ* was CO 2 compensation point inside chloroplast. R d and Γ* were calculated according to a previous study [51]. Briefly, P n -C i curves were measured at two light density(75 and 500 μmol m -2 s -1 ) at CO 2 concentration of 30 to 120 μmol CO 2 mol -1 air. Γ* (x-axis) and Rd (y-axis) was derived according to intersection point of P n -C i curves. J was the electron transport rate, were calculated as described by a previous study [52].
According to the series circuit, the total CO 2 diffusion resistance (1/g tot ) can be determined as [7]: 1/g tot =1/g s +1/g m . Therefore, g tot can be determined as: 14 By definition, L s + L m + L b =1; əA/əC c was determined as the slope of P n -C c curves at CO 2 concentrations of 40~110μmol mol −1 .

Determination of plant water status
Once photosynthetic measurements were completed, leaflets were harvested for determination of plant water status. Leaf water potential (ψ leaf ) was measured by a pressure chamber (PMS-1000, Corvallis, OR, USA). Some plants were kept in dark condition for about 8~10 h for the determination of soil water potential (Ψ soil ) [53]. Since water movement was approximate to zero under dark condition, and thereby Ψ soil remained relative constant and can be assumed to equal the xylem pressure potential of leaf at dark condition.

Leaf morphology
After determination of photosynthesis and water status, leaflets area was measured by leaf area meter. The leaflets samples were dried at 80°C by oven to constant dry mass and weighted. Leaf mass area (LMA) was determined as the ratio of leaf dry mass to leaf area. Abbreviations VPD: Vapour pressure deficit; Ψ leaf : leaf water potential; Ψ soil : soil water potential; Ψ air : air water; potential; ΔΨ leaf-air : the drawdown of water potential between leaf and air; ΔΨ soil-leaf : the drawdown of water potential between soil and leaf ; V cmax : Maximum carboxylation rate ; J max : maximum electron transport rate ; CE: carboxylation efficiency ; g s : stomatal conductance ; g m : mesophyll conductance ; g tot : total conductance; C a : ambient CO 2 concentration; C i : CO 2 concentration of per area, CO 2 , and irradiance on mesophyll conductance in sclerophylls. J. Exp. Bot.    Fig.S3. A simplified pathway for photosynthetic CO 2 uptake and transport. C a , C i and C c represent 22 the CO 2 concentration of air, intercellular and carboxylation site; g s and g m represent stomatal and mesophyll conductance for CO 2 diffusion, respectively; g tot represent the total conductance summing stomatal and mesophyll resistance in series.      Correlations between gm versus gs (A), gs versus Ψ leaf (B), and gm versus Ψ leaf (C). Supplementary.pdf