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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Plant Sci.</journal-id>
<journal-title>Frontiers in Plant Science</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Plant Sci.</abbrev-journal-title>
<issn pub-type="epub">1664-462X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fpls.2023.1116367</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Plant Science</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Photoacclimation and entrainment of photosynthesis by fluctuating light varies according to genotype in <italic>Arabidopsis thaliana</italic>
</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Burgess</surname>
<given-names>Alexandra J.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="author-notes" rid="fn001">
<sup>*</sup>
</xref>
<xref ref-type="author-notes" rid="fn003">
<sup>&#x2020;</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/359078"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Retkute</surname>
<given-names>Renata</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="author-notes" rid="fn001">
<sup>*</sup>
</xref>
<xref ref-type="author-notes" rid="fn003">
<sup>&#x2020;</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/359225"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Murchie</surname>
<given-names>Erik H.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/358526"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>School of Biosciences, University of Nottingham</institution>, <addr-line>Loughborough</addr-line>, <country>United Kingdom</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Department of Plant Sciences, University of Cambridge</institution>, <addr-line>Cambridge</addr-line>, <country>United Kingdom</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>Edited by: Shizue Matsubara, Forschungszentrum J&#xfc;lich, Germany</p>
</fn>
<fn fn-type="edited-by">
<p>Reviewed by: Giles Nicholas Johnson, The University of Manchester, United Kingdom; Carmen Arena, University of Naples Federico II, Italy</p>
</fn>
<fn fn-type="corresp" id="fn001">
<p>*Correspondence: Alexandra J. Burgess, <email xlink:href="mailto:Alexandra.Burgess@nottingham.ac.uk">Alexandra.Burgess@nottingham.ac.uk</email>; Renata Retkute, <email xlink:href="mailto:rr614@cam.ac.uk">rr614@cam.ac.uk</email>
</p>
</fn>
<fn fn-type="equal" id="fn003">
<p>&#x2020;These authors have contributed equally to this work</p>
</fn>
<fn fn-type="other" id="fn002">
<p>This article was submitted to Crop and Product Physiology, a section of the journal Frontiers in Plant Science</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>09</day>
<month>03</month>
<year>2023</year>
</pub-date>
<pub-date pub-type="collection">
<year>2023</year>
</pub-date>
<volume>14</volume>
<elocation-id>1116367</elocation-id>
<history>
<date date-type="received">
<day>05</day>
<month>12</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>10</day>
<month>02</month>
<year>2023</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2023 Burgess, Retkute and Murchie</copyright-statement>
<copyright-year>2023</copyright-year>
<copyright-holder>Burgess, Retkute and Murchie</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>Acclimation of photosynthesis to light intensity (photoacclimation) takes days to achieve and so naturally fluctuating light presents a potential challenge where leaves may be exposed to light conditions that are beyond their window of acclimation. Experiments generally have focused on unchanging light with a relatively fixed combination of photosynthetic attributes to confer higher efficiency in those conditions. Here a controlled LED experiment and mathematical modelling was used to assess the acclimation potential of contrasting Arabidopsis thaliana genotypes following transfer to a controlled fluctuating light environment, designed to present frequencies and amplitudes more relevant to natural conditions. We hypothesize that acclimation of light harvesting, photosynthetic capacity and dark respiration are controlled independently. Two different ecotypes were selected, Wassilewskija-4 (Ws), Landsberg erecta (Ler) and a GPT2 knock out mutant on the Ws background (gpt2-), based on their differing abilities to undergo dynamic acclimation i.e. at the sub-cellular or chloroplastic scale. Results from gas exchange and chlorophyll content indicate that plants can independently regulate different components that could optimize photosynthesis in both high and low light; targeting light harvesting in low light and photosynthetic capacity in high light. Empirical modelling indicates that the pattern of &#x2018;entrainment&#x2019; of photosynthetic capacity by past light history is genotype-specific. These data show flexibility of photoacclimation and variation useful for plant improvement.</p>
</abstract>
<kwd-group>
<kwd>photosynthesis</kwd>
<kwd>acclimation</kwd>
<kwd>induction</kwd>
<kwd>fluctuating light</kwd>
<kwd>entrainment (light)</kwd>
<kwd>
<italic>Arabidopsis thaliana</italic>
</kwd>
</kwd-group>
<contract-sponsor id="cn001">UK Research and Innovation<named-content content-type="fundref-id">10.13039/100014013</named-content>
</contract-sponsor>
<contract-sponsor id="cn002">Leverhulme Trust<named-content content-type="fundref-id">10.13039/501100000275</named-content>
</contract-sponsor>
<counts>
<fig-count count="7"/>
<table-count count="0"/>
<equation-count count="4"/>
<ref-count count="65"/>
<page-count count="12"/>
<word-count count="6913"/>
</counts>
</article-meta>
</front>
<body>
<sec id="s1" sec-type="intro">
<label>1</label>
<title>Introduction</title>
<p>A potential limitation to plant growth under natural conditions is their ability to acclimate to fluctuating light and the speed at which this acclimation occurs. Within natural environments, light intensities constantly fluctuate as a result of changes in solar angle, seasonal variation, passing clouds or movement of overlapping foliage (<xref ref-type="bibr" rid="B10">Burgess et&#xa0;al., 2019</xref>; <xref ref-type="bibr" rid="B59">Wang et&#xa0;al., 2020</xref>; <xref ref-type="bibr" rid="B9">Burgess et&#xa0;al., 2021</xref>). These fluctuations occur over different timescales, although have been shown to occur as rapidly as sub-second (<xref ref-type="bibr" rid="B15">de Langre, 2008</xref>; <xref ref-type="bibr" rid="B9">Burgess et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B19">Durand et&#xa0;al., 2021</xref>). However, natural shade cast by overhead leaves or cloud cover does not only differ in intensity, but also in spectral quality. This shade often has a reduced red: far red ratio and is deficient in photosynthetically active radiation (PAR: 400-700 nm) due to selective filtering by photosynthetic pigments (<xref ref-type="bibr" rid="B32">Murchie and Horton, 1997</xref>; <xref ref-type="bibr" rid="B47">Smith et&#xa0;al., 2017</xref>). This creates a complex challenge for the photosynthetic machinery, with the signals and pathways underlying response poorly understood. Plants have evolved a number of mechanisms to cope with fluctuations in the light environment. These enable the efficient capture and use of light at low irradiance, and avoid damage to photosynthetic machinery at high irradiance (<xref ref-type="bibr" rid="B55">Walters, 2005</xref>; <xref ref-type="bibr" rid="B17">Demmig-Adams et&#xa0;al., 2012</xref>; <xref ref-type="bibr" rid="B43">Ruban, 2017</xref>). However, leaf photosynthesis does not respond instantaneously to a sudden change in light, and there is often a delay before steady state is reached. The length of this delay is closely linked to the photosynthetic induction state, which is a physiological condition dependent on recent light history (<xref ref-type="bibr" rid="B44">Sassenrath-Cole and Pearcy, 1994</xref>; <xref ref-type="bibr" rid="B49">Stegemann et&#xa0;al., 1999</xref>). The induction state is dependent on a number of different processes including photoprotection (<xref ref-type="bibr" rid="B23">Hubbart et&#xa0;al., 2012</xref>), the activation state of photosynthetic enzymes (<xref ref-type="bibr" rid="B62">Yamori et&#xa0;al., 2012</xref>; <xref ref-type="bibr" rid="B13">Carmo-Silva and Salvucci, 2013</xref>; <xref ref-type="bibr" rid="B1">Acevedo-Siaca et&#xa0;al., 2020</xref>) and stomatal dynamics (<xref ref-type="bibr" rid="B26">Lawson and Blatt, 2014</xref>; <xref ref-type="bibr" rid="B28">Long et&#xa0;al., 2022</xref>). However, regardless of induction state, the photosynthetic machinery is able to acclimate (termed photosynthetic acclimation or photoacclimation) to differences in the intensity and spectral composition of light.</p>
<p>Although often referred to as a single process, photosynthetic acclimation involves multiple processes across molecular, cellular and anatomical scales that are often distinct (<xref ref-type="bibr" rid="B6">Athanasiou et&#xa0;al., 2010</xref>). Acclimation refers to changes in the composition and organization of photosynthetic apparatus and can be broadly split into two processes: developmental acclimation and dynamic acclimation (<xref ref-type="bibr" rid="B55">Walters, 2005</xref>). Despite originating from distinct mechanisms, they may overlap in terms of photosynthesis phenotype. Developmental acclimation describes changes to cell size, number and shape and is set early during development. This can arise as different leaves are exposed to varying light levels; as such they optimize photosynthetic efficiency according to the light environment in which they are exposed. Differences in developmental acclimation state can be seen as changes in the characteristics of the light response curve of photosynthesis. Leaves that developed under a higher light level will have a higher maximum photosynthesis rate (<italic>P<sub>max</sub>
</italic>). However, leaves that developed under lower light levels will have a lower light compensation point (LCP). This functions to improve carbon gain at low light intensities, resulting in a shorter, but more sensitive, light-limiting state, thus allowing improved exploitation of low light levels and a swift response to any influx of light due to a passing sun fleck or change in light availability (<xref ref-type="bibr" rid="B64">Yin and Johnson, 2000</xref>; <xref ref-type="bibr" rid="B9">Burgess et&#xa0;al., 2021</xref>). Differences are observed due to changes in chlorophyll concentration, leaf thickness and molecular alterations such as changes in photosystem I (PSI) and photosystem II (PSII) structure and concentration plus changes in photosynthetic enzyme activities (<xref ref-type="bibr" rid="B32">Murchie and Horton, 1997</xref>; <xref ref-type="bibr" rid="B55">Walters, 2005</xref>).</p>
<p>The second form of acclimation is dynamic acclimation, which can be characterized as structural and biochemical changes in the photosynthetic machinery of a mature leaf <xref ref-type="bibr" rid="B56">Walters and Horton (1994)</xref>. It involves reversible responses to light, encompassing changes in the expression of genes and concentration of enzymes which result in alterations in phenotype following an irradiance increase or decrease (<xref ref-type="bibr" rid="B29">M&#xfc;ller et&#xa0;al., 2001</xref>; <xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B52">Townsend et&#xa0;al., 2018</xref>). Responses include changes to PSI and PSII levels or structure; changes in the regulation of electron transport components; changes in enzyme concentrations such as Rubisco and ATPase; changes in granal stacking, changes in stomatal conductance and; the chloroplast avoidance/accumulative response (<xref ref-type="bibr" rid="B56">Walters and Horton, 1994</xref>; <xref ref-type="bibr" rid="B5">Anderson et&#xa0;al., 1995</xref>; <xref ref-type="bibr" rid="B32">Murchie and Horton, 1997</xref>; <xref ref-type="bibr" rid="B58">Walters et&#xa0;al., 1999</xref>; <xref ref-type="bibr" rid="B55">Walters, 2005</xref>; <xref ref-type="bibr" rid="B27">Li et&#xa0;al., 2009</xref>; <xref ref-type="bibr" rid="B20">Dyson et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B30">Matthews et&#xa0;al., 2018</xref>). As such, full dynamic acclimation may take 7 days (<xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>). Dynamic acclimation can also effect the pigment composition found in a leaf, and adaptations to changes in irradiance can manifest themselves as changes in chlorophyll content and ratios. Chlorophyll <italic>a</italic> is found in the reaction center of both photosystems, and its synthesis is dependent on the synthesis of photosystems, whereas chlorophyll <italic>b</italic> is an accessory pigment, part of the antenna complex and therefore is more readily synthesized when light levels drop in an attempt to harvest maximum light (<xref ref-type="bibr" rid="B3">Anderson, 1980</xref>; <xref ref-type="bibr" rid="B4">Anderson, 1986</xref>; <xref ref-type="bibr" rid="B32">Murchie and Horton, 1997</xref>; <xref ref-type="bibr" rid="B58">Walters et&#xa0;al., 1999</xref>). Analysis of chlorophyll content and ratios can provide an alternative to analysis of dark respiration rates, which can be difficult to accurately measure (<xref ref-type="bibr" rid="B57">Walters et&#xa0;al., 2004</xref>). Dynamic acclimation can also be seen through changes to the light response curve characteristics, particularly the impact on <italic>P<sub>max</sub>
</italic>.</p>
<p>The capacity for plants to undergo developmental or dynamic acclimation is species, or genotype, specific (<xref ref-type="bibr" rid="B32">Murchie and Horton, 1997</xref>; <xref ref-type="bibr" rid="B60">Watling et&#xa0;al., 1997</xref>; <xref ref-type="bibr" rid="B34">Murchie et&#xa0;al., 2005</xref>; <xref ref-type="bibr" rid="B6">Athanasiou et&#xa0;al., 2010</xref>). Previously studies on <italic>Arabidopsis thaliana</italic> show accession-, or ecotype-, specific differences in acclimation capacity (<xref ref-type="bibr" rid="B6">Athanasiou et&#xa0;al., 2010</xref>). This confers plant fitness under fluctuating light with the popular accession Colombia (Col) exhibiting an inability to undergo dynamic acclimation. Furthermore, <xref ref-type="bibr" rid="B6">Athanasiou et&#xa0;al. (2010)</xref> identified the gene At1g61800, encoding a glucose-6-phosphate/phosphate translocator- GPT2, as integral to ability to dynamically activate. GPT2 is thought to mediate dynamic acclimation responses <italic>via</italic> metabolic fluxes. It is responsible for the import of glucose-6-phosphate (G6P) from the cytosol into the chloroplast (<xref ref-type="bibr" rid="B25">Kunz et&#xa0;al., 2010</xref>). This has the net effect of increasing starch synthesis, resulting in an increase in chloroplastic phosphate concentration, leading to gene expression changes which allow the cell to sense changes in environmental signals (<xref ref-type="bibr" rid="B55">Walters, 2005</xref>; <xref ref-type="bibr" rid="B20">Dyson et&#xa0;al., 2015</xref>). Whilst <italic>gpt2</italic> knock out mutants grow normally, and demonstrate developmental acclimation (<xref ref-type="bibr" rid="B36">Niewiadomski et&#xa0;al., 2005</xref>), they do not exhibit dynamic acclimation (<xref ref-type="bibr" rid="B20">Dyson et&#xa0;al., 2015</xref>), which means they can provide a negative control for demonstrating the fitness benefits of dynamic acclimation in <italic>Arabidopsis</italic>.</p>
<p>Both developmental and dynamic acclimation are important under natural conditions but knowledge of how they interact together is poorly understood. Fluctuating light presents a potential challenge to the acclimation process: a high light acclimated leaf will not perform well under low light and vice versa. This is partly as a result of constraints imposed by the anatomy of the leaf (<xref ref-type="bibr" rid="B38">Oguchi et&#xa0;al., 2003</xref>), as well as the correlation between photosynthetic capacity and dark respiration (<xref ref-type="bibr" rid="B21">Givnish, 1988</xref>; <xref ref-type="bibr" rid="B37">Niinemets and Tenhunen, 1997</xref>; <xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>). Therefore, should a plant exploit high light <italic>via</italic> raising <italic>P<sub>max</sub>
</italic> and/or should a plant enhance light capture and reduce respiratory loss under low light? There has been extensive research on how plants acclimate to high- and low- light (<xref ref-type="bibr" rid="B3">Anderson, 1980</xref>; <xref ref-type="bibr" rid="B4">Anderson, 1986</xref>; <xref ref-type="bibr" rid="B16">Demmig-Adams and Adams, 1992</xref>; <xref ref-type="bibr" rid="B32">Murchie and Horton, 1997</xref>; <xref ref-type="bibr" rid="B64">Yin and Johnson, 2000</xref>; <xref ref-type="bibr" rid="B57">Walters et&#xa0;al., 2004</xref>; <xref ref-type="bibr" rid="B45">Scheibe et&#xa0;al., 2005</xref>; <xref ref-type="bibr" rid="B55">Walters, 2005</xref>; <xref ref-type="bibr" rid="B6">Athanasiou et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B25">Kunz et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B50">Suorsa et&#xa0;al., 2012</xref>; <xref ref-type="bibr" rid="B20">Dyson et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>), however, few experiments have focused on the effect of controlled fluctuating light (<xref ref-type="bibr" rid="B14">Chabot et&#xa0;al., 1979</xref>; <xref ref-type="bibr" rid="B60">Watling et&#xa0;al., 1997</xref>; <xref ref-type="bibr" rid="B64">Yin and Johnson, 2000</xref>; <xref ref-type="bibr" rid="B54">Vialet-Chabrand et&#xa0;al., 2017</xref>; <xref ref-type="bibr" rid="B30">Matthews et&#xa0;al., 2018</xref>). Of those that have been carried out, experiments have predominantly used fluctuating light patterns that alternate between a fixed high and low value, with exceptions e.g. <xref ref-type="bibr" rid="B54">Vialet-Chabrand et&#xa0;al. (2017)</xref>, thus they do not represent the varying irradiances that plants are subject to in the natural environment.</p>
<p>Recent research has focused more on the short term metabolic efficiencies of photosynthesis during light switches without the &#x2018;background&#x2019; shifts in long term changes in composition and this has effects on canopy productivity (<xref ref-type="bibr" rid="B28">Long et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B48">Souza et&#xa0;al., 2022</xref>). During the shift from low to high light, the &#x2018;induction state&#x2019; of photosynthesis determines the rate of response and is governed by enzyme activation state and stomatal aperture. The induction state is in turn determined by the length of time spent in high or low light - the leaf &#x2018;light history&#x2019; or entrainment. We currently have limited information on genetic variation of entrainment although a recent study showed variation in deactivation state of Rubisco (<xref ref-type="bibr" rid="B51">Taylor et&#xa0;al., 2022</xref>). Furthermore, it is understood that the maximum photosynthetic capacity of a plant is dependent on the number of switches between high and low light intensity and the proportion of time spent under each irradiance (<xref ref-type="bibr" rid="B64">Yin and Johnson, 2000</xref>; <xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>). For example, the more time recently spent in high light, the faster the induction response due to the persistence of metabolic and physiological processes that favor photosynthesis such as Rubisco activation state and stomatal conductance. Thus both photoacclimation and entrainment of photosynthesis determine the overall plant response. However there have been few approaches to understand how this can be measured or modelled (<xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>). Until recently, producing accurate fluctuations of light were not possible but lightemitting diode- (LED) based growth chambers enable us to subject plants to a predetermined and controlled pattern of irradiance.</p>
<p>This study addresses two unknown aspects of acclimation. We hypothesized that (1) <italic>Arabidopsis</italic> will engage separate high (photosynthetic capacity) and low (light harvesting and respiration) acclimation responses in a fluctuating light regime and (2) the entrainment of induction state differs between <italic>Arabidopsis</italic> genotypes. We approach this by studying contrasting genotypes of <italic>Arabidopsis</italic> that have varying acclimation responses. After transfer to fluctuating light we measured photosynthetic light response curves and chlorophyll composition. We compared these data to our dynamic model of acclimation (<xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>). We show the existence of separate acclimation responses in fluctuating light that optimize light harvesting and quantum yield at low and capacity under high light while rate of entrainment of induction state by light history varies between accessions.</p>
</sec>
<sec id="s2" sec-type="materials|methods">
<label>2</label>
<title>Materials and methods</title>
<sec id="s2_1">
<label>2.1</label>
<title>Plant growth</title>
<p>
<italic>A. thaliana</italic> ecotypes Landsberg erecta (Ler), Wassilewskija (Ws) and a <italic>gpt2-</italic> mutant (Ws WT background) were selected based on their differing abilities to undergo dynamic acclimation (<xref ref-type="bibr" rid="B6">Athanasiou et&#xa0;al., 2010</xref>) The seeds were vernalized at 4&#xb0;C in a water suspension for 48 hours, prior to transfer into 6.5 cm diameter pots containing Levington M3 compost. One week after germination, seedlings were transplanted into individual pots containing 25 g of Levington M3 compost. Plants were cultivated in a Fytoscope 3000 (Photon System Instruments, PSI, Czech Republic) growth chamber, which uses a combination of red and blue LEDs (1:1 ratio throughout on a photon flux basis) plus far-red LEDs (set to a constant 10 <italic>&#xb5;mol m</italic>
<sup>-2</sup> s<sup>-1</sup> throughout the day). The cabinet was set to a 12 hour photoperiod, with a 20&#xb0;C day temperature, 16&#xb0;C night temperature and 50% relative humidity; these conditions remained constant throughout the experiment.</p>
</sec>
<sec id="s2_2">
<label>2.2</label>
<title>Light treatments</title>
<p>Plants were split into two groups and were subject to two different light treatments: Constant light (CL) and fluctuating light (FL). The CL plants were grown under 266 &#xb1; 10 <italic>&#xb5;mol m</italic>
<sup>-2</sup>
<italic>s</italic>
<sup>-1</sup> for the duration of the experiment, i.e. up to 37 days. This constant pattern included an initial ramp up and final ramp down stage to represent sunrise and sunset, respectively. The FL group was subject to constant light for 28 days and then transferred into a fluctuating light for the remainder of experiment (i.e. 9 days). 9 days was selected to ensure full dynamic acclimation (<xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>). During growth, plants were kept well-watered. The experiment was repeated four times for Ws and <italic>gpt2-</italic> and three times for Ler.</p>
<p>Due to the short growth span of <italic>Arabidopsis</italic>, response to the FL treatment represents a combination of developmental and dynamic acclimation, where growth for the first 28 days was under a constant light.</p>
<p>The fluctuating light pattern was designed as a re-occurring 3 h 20 min light motif, which was repeated 3 times throughout the day, combined with an initial ramp up and final ramp down phase (<xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1</bold>
</xref>). Each light step was a minimum of 20 min long to discount changes as a result of induction. Care was taken to accommodate different steps in light intensity, decreasing from 400 <italic>&#xb5;mol m</italic>
<sup>-2</sup>
<italic>s</italic>
<sup>-1</sup> to 100 <italic>&#xb5;mol m</italic>
<sup>-2</sup>
<italic>s</italic>
<sup>-1</sup> or increasing from 50 <italic>&#xb5;mol m</italic>
<sup>-2</sup>
<italic>s</italic>
<sup>-1</sup> to 400 <italic>&#xb5;mol m</italic>
<sup>-2</sup>
<italic>s</italic>
<sup>-1</sup>. Overall, the fluctuating light pattern had the same daily integrated photon dose as the constant light pattern.</p>
<fig id="f1" position="float">
<label>Figure&#xa0;1</label>
<caption>
<p>Light patterns used for the analysis of acclimation in <italic>Arabidopsis thaliana</italic>. Plants were split into two groups and were subject to two different light treatments: Constant Light (CL: red) versus Fluctuating Light (FL: black).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-14-1116367-g001.tif"/>
</fig>
</sec>
<sec id="s2_3">
<label>2.3</label>
<title>Physiological measurements</title>
<p>Both destructive and non-destructive measurements were made on plants. Analysis of rosette area was performed on all plants starting at 21 days after sowing (DAS). Plants were briefly removed from the Fytoscope 3000 growth cabinet into the adjoining room every other working day and were photographed using a RGB camera (Canon EOS 650D SLR, Canon Europa N.V., The Netherlands) using ambient lighting and a scale. Images were analyzed using Image J for rosette area (<xref ref-type="bibr" rid="B46">Schneider et&#xa0;al., 2012</xref>).</p>
<p>We assumed that increases in the size of plants followed the exponential growth as a function of time:</p>
<disp-formula>
<label>(1)</label>
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<mml:mrow>
<mml:mi>A</mml:mi>
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<mml:mi>e</mml:mi>
<mml:mi>a</mml:mi>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mi>d</mml:mi>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mo>=</mml:mo>
<mml:msub>
<mml:mi>a</mml:mi>
<mml:mn>0</mml:mn>
</mml:msub>
<mml:msup>
<mml:mrow>
<mml:mi>exp</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>a</mml:mi>
<mml:mn>1</mml:mn>
</mml:msub>
<mml:mi>d</mml:mi>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>d</italic> is a day from sowing, and <italic>a</italic>
<sub>1</sub> is relative growth rate. Curve fitting for rosette area was carried out using Mathematica (Wolfram, UK).</p>
<p>Following gas exchange measurements (see below), chlorophyll assays were carried out. A size 4 leaf borer was used to take 2 leaf discs per plant from leaves in the 3rd whorl, which were placed immediately in cold, 80% acetone and kept dark. Leaf samples were ground in 80% acetone and made up to 5 ml before being centrifuged for 5 min at 3000 r.p.m, 1600 g. The chlorophyll content and a:b ratios in the supernatant was determined according to (<xref ref-type="bibr" rid="B40">Porra et&#xa0;al., 1989</xref>) using absorption with a spectrophotometer at 646.6, 663.6 and 750 <italic>nm</italic>.</p>
</sec>
<sec id="s2_4">
<label>2.4</label>
<title>Gas exchange measurements</title>
<p>Whole plant light response curves (LRCs) were taken using the LI-COR 6400XT (Li-COR, Nebraska, USA) using the whole plant chamber attachment (6400-17) and RGB Light source (6400-18A for LRCS) at the end of the experiment (36 DAS+). The small size of some of the leaves precluded the use of the standard LI-COR 6400XT chamber, and measurement of the whole plant allows the response of both developmental and dynamic acclimation to be monitored. For all gas exchange measurements, plants were not dark-adapted prior to measurements. The block temperature was maintained at 20&#xb0;C using a flow rate of 600 l <italic>min<sup>-1</sup>
</italic>. For LRCs, light was provided by a combination of in-built red, blue and green LEDs, set to &#x2018;white&#x2019; light. Illumination occurred over a series of 12 PAR values between 0 and 1500 <italic>&#xb5;mol m</italic>
<sup>-2</sup>
<italic>s</italic>
<sup>-1</sup>, with a minimum of two minutes at each light level. At least 6 replicates were taken per experimental repeat for both CL and FL plants.</p>
<p>During the FL treatment period, changes in photosynthesis were measured using the LI-COR 6400XT with the whole plant chamber attachment and sun and sky lid. An &#x2018;autologging&#x2019; program was created that took measurements every 15 seconds throughout the FL. The LI-COR was placed inside the Fytoscope chamber, with the chamber providing the light pattern to the individual plant being measured through the sun and sky lid. <italic>CO</italic>
<sub>2</sub> was maintained at 400 p.p.m. throughout. Due to the repeating light signature (3 hours 20 minutes long; see Materials and Methods, Plant Growth), 3 replicates were taken per day on days 1, 3, 5 and 8- post treatment (corresponding to 28, 30, 32 and 35 DAS). Autologging was carried out for two full repeat experiments of the WTs Ler and Ws (i.e. 6 replicates per post treatment day) and one full experiment for the <italic>gpt2-</italic> mutant. The data was normalized according to the average photosynthesis during the last 10 time points at the end of the light pattern and then averaged.</p>
</sec>
<sec id="s2_5">
<label>2.5</label>
<title>Light response curve fitting</title>
<p>Curve fitting for LRCs was carried out using the Mathematica (Wolfram, UK). The net photosynthetic rate, or assimilation, <italic>A</italic>, as a function of irradiance, <italic>L</italic>, can be described using the non-rectangular hyperbola [41]:</p>
<disp-formula>
<label>(2)</label>
<mml:math display="block" id="M2">
<mml:mrow>
<mml:mi>A</mml:mi>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mi>L</mml:mi>
<mml:mo>,</mml:mo>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>,</mml:mo>
<mml:mi>&#x3b1;</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>&#x3b8;</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>&#x3d5;</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mo>=</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mi>&#x3d5;</mml:mi>
<mml:mi>L</mml:mi>
<mml:mo>+</mml:mo>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>+</mml:mo>
<mml:mi>&#x3b1;</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msqrt>
<mml:mrow>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mi>&#x3d5;</mml:mi>
<mml:mi>L</mml:mi>
<mml:mo>+</mml:mo>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>+</mml:mo>
<mml:mi>&#x3b1;</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
<mml:msup>
<mml:mo stretchy="false">)</mml:mo>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>4</mml:mn>
<mml:mi>&#x3b8;</mml:mi>
<mml:mi>&#x3d5;</mml:mi>
<mml:mi>L</mml:mi>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>+</mml:mo>
<mml:mi>&#x3b1;</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:msqrt>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:mi>&#x3b8;</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>&#x3b1;</mml:mi>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</disp-formula>
<p>The nonrectangular hyperbola is defined by four parameters: the quantum use efficiency (QY), <italic>&#x3d5;</italic>; convexity, <italic>&#x3b8;</italic>; maximum photosynthetic capacity, <italic>P<sub>max</sub>
</italic> and; the rate of dark respiration, <italic>R<sub>d</sub>
</italic>. We assumed that the rate of dark respiration is proportional to the maximum photosynthetic capacity, according to the relationship <italic>R<sub>d</sub>
</italic> = &#x3b1;<italic>P<sub>max</sub>
</italic> (<xref ref-type="bibr" rid="B22">Givnish and Vermeij, 1976</xref>; <xref ref-type="bibr" rid="B37">Niinemets and Tenhunen, 1997</xref>; <xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>). Fitting was performed using the Mathematica command &#x2018;FindFit&#x2019; with a minimum constraint on dark respiration at 0.05 and convexity at 0.8.</p>
</sec>
<sec id="s2_6">
<label>2.6</label>
<title>Modelling the photosynthetic response</title>
<p>A model incorporating a &#x2018;fading memory&#x2019; of the recent light pattern in the form of a time-weighted average for the light was introduced in (<xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>):</p>
<disp-formula>
<label>(3)</label>
<mml:math display="block" id="M3">
<mml:mrow>
<mml:msub>
<mml:mi>L</mml:mi>
<mml:mi>&#x3c4;</mml:mi>
</mml:msub>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mi>t</mml:mi>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mo>=</mml:mo>
<mml:mfrac>
<mml:mn>1</mml:mn>
<mml:mi>&#x3c4;</mml:mi>
</mml:mfrac>
<mml:munderover>
<mml:mo>&#x222b;</mml:mo>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>&#x221e;</mml:mi>
</mml:mrow>
<mml:mi>t</mml:mi>
</mml:munderover>
<mml:mi>L</mml:mi>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:msup>
<mml:mi>t</mml:mi>
<mml:mo>&#x2032;</mml:mo>
</mml:msup>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:msup>
<mml:mi>e</mml:mi>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mi>t</mml:mi>
<mml:mo>&#x2032;</mml:mo>
</mml:msup>
</mml:mrow>
<mml:mi>&#x3c4;</mml:mi>
</mml:mfrac>
</mml:mrow>
</mml:msup>
<mml:mi>d</mml:mi>
<mml:msup>
<mml:mi>t</mml:mi>
<mml:mo>&#x2032;</mml:mo>
</mml:msup>
</mml:mrow>
</mml:math>
</disp-formula>
<p>This describes the ability for plants to respond more strongly to recent changes in light history. This effectively accounts for photosynthetic induction state, which is very hard to quantify <italic>in situ</italic> as it varies according to the light history of the leaf.</p>
<p>This fading memory was incorporated into the light response functions when calculating instantaneous photosynthetic rate, <italic>P</italic>, at a time <italic>t</italic>. The model was adapted so the time-weighted average was only applied during the transition from low to highlight (to represent induction) but not from high to low light, during which photosynthesis can almost immediately respond.</p>
<disp-formula>
<label>(4)</label>
<mml:math display="block" id="M4">
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>&#x3c4;</mml:mi>
<mml:mo>,</mml:mo>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>,</mml:mo>
<mml:mi>&#x3b1;</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>&#x3b8;</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>&#x3d5;</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mo>=</mml:mo>
<mml:mi>A</mml:mi>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mi>min</mml:mi>
<mml:mtext>&#xa0;</mml:mtext>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mi>L</mml:mi>
<mml:mi>&#x3c4;</mml:mi>
</mml:msub>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mi>t</mml:mi>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mo>,</mml:mo>
<mml:mi>L</mml:mi>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mi>t</mml:mi>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mo>,</mml:mo>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>,</mml:mo>
<mml:mi>&#x3b1;</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>&#x3b8;</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>&#x3d5;</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:math>
</disp-formula>
<p>We estimated distributions of &#x3c4;, <italic>P<sub>max</sub>
</italic>, &#x3b1;, &#x3b8; and &#x3d5; for each accession and each day. Parameters were fitted using adaptive multiple importance sampling (<xref ref-type="bibr" rid="B42">Retkute et&#xa0;al., 2021</xref>) with likelihood formulated assuming normally distributed errors between photosynthetic rate measured in the experiments and simulated using Eq.4. Parameter prior distributions were assumed to be uniform within following ranges: &#x3c4; &#x3f5; [0,60], <italic>P<sub>max</sub>
</italic> &#x3f5; [0,30], &#x3b1; &#x3f5; [0.03,1], <italic>&#x3d5;</italic> &#x3f5; [0,1] and <italic>&#x3b8;</italic> &#x3f5; [0.6,0.99].</p>
</sec>
<sec id="s2_7">
<label>2.7</label>
<title>Statistical analysis</title>
<p>Analysis of variance (ANOVA) was carried out using GenStat for Windows, 17th Edition (VSN International Ltd.). An unbalanced design was used to account for differences in the number of replicates each round (i.e. due to plant mortality). The data was checked to see if it met the assumption of constant variance and normal distribution of residuals. For all statistical analyses, data from each of the lines (Ws, Ler and <italic>gpt2-</italic>) were treated independently because of their differing responses to a change in light. Rosette area was analyzed at 28 DAS and 37 DAS. The former was carried out to ensure that plant growth was same in the CL treatment relative to FL treatment during the period of growth under which they were subject to the same light pattern (grey horizontal line; <xref ref-type="fig" rid="f1">
<bold>Figure&#xa0;1</bold>
</xref>) whilst the latter was to determine whether the fluctuating light pattern influenced growth and final rosette area. Chlorophyll <italic>a</italic>:<italic>b</italic> ratio, total chlorophyll content and length of memory fading window were analyzed using ANOVAs.</p>
</sec>
</sec>
<sec id="s3" sec-type="results">
<label>3</label>
<title>Results</title>
<sec id="s3_1">
<label>3.1</label>
<title>Fluctuating light and plant growth</title>
<p>Rosette area of each accession under CL and FL during the course of the experiment is given in <xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2</bold>
</xref>. Whilst this does not account for overlapping leaves or leaf thickness, it can be used as an approximation of growth rate. Two treatment comparisons were performed on each accession in order to see if there were any differences in growth of the plants: first at 28 DAS to ensure consistent growth prior to FL treatment and; secondly at the end of the experiment (37 DAS). At 28 DAS there was no significant difference in rosette area between the treatments in any line, which suggests that up to that point the plants grew similarly. Similarly, at 37 DAS there was no significant difference in the rosette area for any line indicating that 9 days of FL did not significantly alter growth. We estimated the relative [visible] leaf area expansion to be between 5.5 and 6.5 <italic>cm</italic>
<sup>2</sup> per day (fitted curves in <xref ref-type="fig" rid="f2">
<bold>Figure&#xa0;2</bold>
</xref>).</p>
<fig id="f2" position="float">
<label>Figure&#xa0;2</label>
<caption>
<p>Rosette area time course. Measurements began 21 days after sowing (DAS) for constant light (red) and fluctuating light (black) plants. Each data point correspond to <italic>n</italic>=4 replicates. For the fluctuating light treatment plants, the light pattern was changed at 28 DAS, as denoted by the grey vertical line. Curves show fitted exponential growth given by Eq. 1.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-14-1116367-g002.tif"/>
</fig>
</sec>
<sec id="s3_2">
<label>3.2</label>
<title>Response of <italic>P<sub>max</sub>
</italic> in <italic>Arabidopsis</italic> under fluctuating light</title>
<p>LRCs indicate a significant increase in <italic>P<sub>max</sub>
</italic> for both the wild type accessions (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref>: Ws p=0.023; Ler p&lt;0.001), indicative of acclimation to high light. In comparison, the <italic>P<sub>max</sub>
</italic> for the <italic>gpt</italic>2- mutant significantly decreased (p=0.013). Direct comparisons between Ws and <italic>gpt</italic>2- under CL showed no significant difference in <italic>P<sub>max</sub>
</italic>. However, under FL, <italic>P<sub>max</sub>
</italic> in the mutant was significantly lower, indicating the importance of <italic>gpt</italic>2- to FL.</p>
<fig id="f3" position="float">
<label>Figure&#xa0;3</label>
<caption>
<p>Light response curves for plants grown under constant light (red) versus fluctuating light (black). Light response curves were measured 35 days after sowing, equivalent to 9 days after starting the fluctuating light pattern (FL plants).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-14-1116367-g003.tif"/>
</fig>
<p>Similar to that seen for <italic>P<sub>max</sub>
</italic>, fitted values indicate that for both the WT accessions, QY was significantly higher in plants under FL compared to those under CL (p&lt;0.001 for Ws and p=0.006 for Ler); a further indicator of high light acclimation. There was no significant difference in QY for <italic>gpt</italic>2- under CL versus FL. There was a significant decrease in LCP in the FL plants for Ws (p=0.012) but not Ler or <italic>gpt</italic>2-. A decrease in LCP is an indicator of acclimation to low light. Ler exhibits an increase in <italic>R<sub>d</sub>
</italic> in fluctuating light, however, no difference in <italic>R<sub>d</sub>
</italic> was found in the other two genotypes.</p>
</sec>
<sec id="s3_3">
<label>3.3</label>
<title>Change in chlorophyll content and <italic>a</italic>:<italic>b</italic> ratio in <italic>Arabidopsis</italic> under fluctuating light</title>
<p>There was no significant difference in chlorophyll <italic>a:b</italic> in Ws, and for both Ler and <italic>gpt</italic>2- the chlorophyll <italic>a:b</italic> ratios were significantly lower in the FL plants compared to the CL plants (p=0.049 and p=0.004, respectively) (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4</bold>
</xref>). Moreover, for both Ws and <italic>gpt</italic>2- the total Chl content was significantly lower in plants under FL compared to those under CL (p&lt;0.001 and p=0.002, respectively). For Ler, no significant change was observed between total Chl amount.</p>
</sec>
<sec id="s3_4">
<label>3.4</label>
<title>Light history effects on acclimation during fluctuating light</title>
<p>The light motif was split into 8 stages according to the irradiance level (Colored bars; <xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4</bold>
</xref>). For stages 1-4 and 6 (corresponding to the light intensity of 400, 100, 200, 50 and 100 <italic>&#xb5;mol m</italic>
<sup>-2</sup>
<italic>s</italic>
<sup>-1</sup>, respectively), the average normalized photosynthesis value of the last 50 time points during the step (i.e. at steady state) was calculated. For stage 5, the time taken to reach a normalized photosynthesis value of 0.7, 0.8 and 0.9 was calculated as a proxy for rate of change. There was no significant difference in days post treatment for any of the lines at stages 1-3 and 6. For <italic>gpt</italic>2- and Ws, there was no significant difference during stage 4 (i.e. the step at 50 <italic>&#xb5;mol m</italic>
<sup>-2</sup>
<italic>s</italic>
<sup>-1</sup>) or 5 (i.e. the step from 50 to 400 <italic>&#xb5;mol m</italic>
<sup>-2</sup>
<italic>s</italic>
<sup>-1</sup>). However, for Ler there was a significant difference (Stage 4, p= 0.017; Stage 5, p=0.044 and p=0.036 for a normalized photosynthesis of 0.8 and 0.9, respectively). This indicates that in the days following a change in the light environment, Ler was able to respond more quickly to a change in irradiance compared to the other genotypes, thus indicating the importance of the light history.</p>
<fig id="f4" position="float">
<label>Figure&#xa0;4</label>
<caption>
<p>Chlorophyll analysis of plants. <bold>(A)</bold> Chlorophyll a:b ratio. <bold>(B)</bold> Total chlorophyll content. Comparisons were made in each case using an unbalanced ANOVA (NS=Not significant; * = p&lt;0.01). Constant light treatment (red) versus fluctuating light treatment (black).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-14-1116367-g004.tif"/>
</fig>
<p>The time-weighted average (Equation (3) acts as a &#x2018;fading memory&#x2019; of the recent light pattern and uses an exponentially decaying weight. If &#x3c4; = 0 then a plant will able to instantaneously respond to a change in irradiance, whereas if &#x3c4;&lt; 0 the time-weighted average light pattern will relax over the timescale &#x3c4;. Previous data from <italic>Arabidopsis</italic> indicates that &#x3c4; &#x2248; 0 hours (<xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>). This value of &#x3c4; (0.3h) represented a maximum leaf &#x2018;memory&#x2019; of around 18 minutes that exponentially declines according to time spent in the light.</p>
<p>For this study, a model, given by Eq.(4), was fit to values of photosynthetic rate during stage 5 of the light motif, i.e. after switching irradiance from 50 <italic>&#xb5;mol m</italic>
<sup>-2</sup>
<italic>s</italic>
<sup>-1</sup> to 400 <italic>&#xb5;mol m</italic>
<sup>-2</sup>
<italic>s</italic>
<sup>-1</sup> (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5</bold>
</xref>; <xref ref-type="supplementary-material" rid="SM1">
<bold>Supplementary Figure S1</bold>
</xref>). This time period was selected because it showed the strongest response to change in irradiance levels. There were statistically significant differences between accessions (p&lt;2e<sup>-16</sup>) and between days (p&lt;2e<sup>-16</sup>). Ler had the highest values of the fading memory window, corresponding to the slowest photosynthetic induction (16.9 - 20.8 minutes; <xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5A</bold>
</xref>). Ler plants showed tendency for decrease in &#x3c4; with more days spend under FL regime, corresponding to an increase in <italic>P<sub>max</sub>
</italic> during the latter days of the experiment (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5B</bold>
</xref>). The length of photosynthetic response for Ws was estimated to be between 13.8 and 16.5 minutes. The fastest response to increase in light intensity was for <italic>gpt2-</italic>. However, the response time increased with number of days spend under FL for both Ws and <italic>gpt2-</italic> (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5A</bold>
</xref>), yet there was still an increase in <italic>P<sub>max</sub>
</italic> during the course of the experiment for <italic>gpt2-</italic> but not the WT Ws. Overall, a good correspondence between the fitted model and experimental measurements was found for all accessions and days (<xref ref-type="supplementary-material" rid="SM1">
<bold>Supplemental Figure S1</bold>
</xref>).</p>
<fig id="f5" position="float">
<label>Figure&#xa0;5</label>
<caption>
<p>Photosynthetic response at days 1, 3, 5 and 8 after switching to FL regime for the three accessions: <bold>(A)</bold> estimated length of photosynthetic response &#x3c4;; <bold>(B)</bold> estimated maximum photosynthetic capacity <italic>P<sub>max</sub>
</italic>.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-14-1116367-g005.tif"/>
</fig>
</sec>
</sec>
<sec id="s4" sec-type="discussion">
<label>4</label>
<title>Discussion</title>
<p>Photosynthetic acclimation to irradiance is known to include changes in leaf anatomy, biochemistry and physiology (<xref ref-type="bibr" rid="B56">Walters and Horton, 1994</xref>; <xref ref-type="bibr" rid="B7">Bailey et&#xa0;al., 2001</xref>; <xref ref-type="bibr" rid="B55">Walters, 2005</xref>). However, many aspects of the process are still unknown and the regulatory steps underlying acclimation are yet to be fully elucidated (<xref ref-type="bibr" rid="B55">Walters, 2005</xref>; <xref ref-type="bibr" rid="B6">Athanasiou et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B54">Vialet-Chabrand et&#xa0;al., 2017</xref>). Transitions from low to high light require photosynthetic induction, including the activation of Rubisco and the opening of stomata (<xref ref-type="bibr" rid="B13">Carmo-Silva and Salvucci, 2013</xref>; <xref ref-type="bibr" rid="B26">Lawson and Blatt, 2014</xref>), whereas transitions from high to low light require the relaxation of dissipative energy processes, collectively known as non-photochemical quenching (NPQ) (<xref ref-type="bibr" rid="B43">Ruban, 2017</xref>; <xref ref-type="bibr" rid="B59">Wang et&#xa0;al., 2020</xref>).</p>
<sec id="s4_1">
<label>4.1</label>
<title>Fluctuating light drives independent responses for different acclimation components</title>
<p>One of the commonly cited functions of acclimation is maintenance of photosynthetic efficiency under the new light regime. For example the lowering of light compensation point, <italic>R<sub>d</sub>
</italic> and antenna size under low light. However naturally fluctuations create a dilemma in which both low light and high light acclimation states would be beneficial during the same photoperiod. How do plants deal with this problem? We argue that these features, often seen as fixed to high light or fixed to low light, are not necessarily in conflict (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6</bold>
</xref>). Low light acclimated leaves can support high photosynthetic rates as long as photoprotective mechanisms are engaged and other stress factors such as high leaf temperature are not present. Up-regulation of electron transport components can induce a higher <italic>P<sub>max</sub>
</italic> during dynamic acclimation without change in Calvin cycle components (<xref ref-type="bibr" rid="B34">Murchie et&#xa0;al., 2005</xref>; <xref ref-type="bibr" rid="B54">Vialet-Chabrand et&#xa0;al., 2017</xref>).</p>
<fig id="f6" position="float">
<label>Figure&#xa0;6</label>
<caption>
<p>A highly schematic figure to summarize the principles arising from this paper. &#x2018;Square wave&#x2019; type growth conditions at a fixed irradiance result in a predictable acclimation condition <bold>(A, C)</bold>. This allows especially high efficiency at these given light levels. Fluctuating conditions, whether natural or imposed, can result in combinations of responses and stoichiometries of the various chloroplast components <bold>(B)</bold>. This is likely to be dependent on the plant, genotype and properties of the imposed light. The cartoon electron transport chain (right pannels) shows the amount of each component proportional with balloon size. In this paper we highlight the possibility of large antenna but high photosynthetic capacity perhaps conferred by higher amounts of electron transport components. This allows the leaf to provide a wider &#x2018;acclimation space&#x2019; and exploit high and low light with higher efficiency than <bold>(A)</bold> or <bold>(C)</bold>.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-14-1116367-g006.tif"/>
</fig>
<p>In consensus with the literature, both WT plants exhibited an increase in <italic>P<sub>max</sub>
</italic> under fluctuation light (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref>) (<xref ref-type="bibr" rid="B32">Murchie and Horton 1997</xref>; <xref ref-type="bibr" rid="B64">Yin and Johnson, 2000</xref>; <xref ref-type="bibr" rid="B55">Walters, 2005</xref>; <xref ref-type="bibr" rid="B27">Li et&#xa0;al., 2009</xref>; <xref ref-type="bibr" rid="B6">Athanasiou et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B20">Dyson et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B54">Vialet-Chabrand et&#xa0;al., 2017</xref>). Increasing <italic>P<sub>max</sub>
</italic> under high light is usually mirrored by a step-wise increase in Chl <italic>a:b</italic> ratio, due to loss of light harvesting complex (LHCII) (<xref ref-type="bibr" rid="B3">Anderson, 1980</xref>; <xref ref-type="bibr" rid="B4">Anderson, 1986</xref>; <xref ref-type="bibr" rid="B32">Murchie and Horton, 1997</xref>; <xref ref-type="bibr" rid="B7">Bailey et&#xa0;al., 2001</xref>; <xref ref-type="bibr" rid="B45">Scheibe et&#xa0;al., 2005</xref>). <xref ref-type="bibr" rid="B54">Vialet-Chabrand et&#xa0;al. (2017)</xref> found that in the accession Col-0, there was an increase in LHCa1 in non-fluctuating conditions, indicating that fluctuating light was inducing a preferential high light response despite the occurrence of low light periods in the regime. Within this study, a lower Chl <italic>a:b</italic> ratio was observed for Ler in the FL treatment compared to CL treatment (<xref ref-type="fig" rid="f7">
<bold>Figure&#xa0;7</bold>
</xref>), this combined with the significant increase in <italic>P<sub>max</sub>
</italic> (<xref ref-type="fig" rid="f3">
<bold>Figure&#xa0;3</bold>
</xref>) plus a change in photosynthesis at 50 <italic>&#xb5;mol m</italic>
<sup>-2</sup>
<italic>s</italic>
<sup>-1</sup> in the days following a change in the light treatment (<xref ref-type="fig" rid="f4">
<bold>Figure&#xa0;4</bold>
</xref>) suggests features of acclimation to both the high- and low- light are present (<xref ref-type="bibr" rid="B3">Anderson, 1980</xref>; <xref ref-type="bibr" rid="B4">Anderson, 1986</xref>; <xref ref-type="bibr" rid="B7">Bailey et&#xa0;al., 2001</xref>; <xref ref-type="bibr" rid="B57">Walters et&#xa0;al., 2004</xref>) (<xref ref-type="fig" rid="f6">
<bold>Figure&#xa0;6</bold>
</xref>). Whilst Chl <italic>a:b</italic> and leaf Chl content were typical of a low light response, <italic>P<sub>max</sub>
</italic> was independent of this. With the exception of Ws, the Chl <italic>a:b</italic> responses indicate acclimation of the antenna to low light, not high light upon transfer to FL. Therefore, chlorophyll traits operated independently to the lack of <italic>P<sub>max</sub>
</italic> acclimation conferred by the <italic>GPT</italic>2 gene. The reduction in chlorophyll content under FL could therefore have been achieved by a reduction in chloroplast number, size or cell size whilst the stromal fraction for Rubisco content increased to confer the higher <italic>P<sub>max</sub>
</italic>. The origin of the higher <italic>P<sub>max</sub>
</italic> would therefore need to be determined.</p>
<fig id="f7" position="float">
<label>Figure&#xa0;7</label>
<caption>
<p>Measured photosynthesis rate in the days following a change in the light pattern. Measurements were made every 15 seconds throughout the light motif at days 1, 3, 5 and 8 post treatment.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-14-1116367-g007.tif"/>
</fig>
<p>Contrary to previous experiments, there was no significant difference in <italic>R<sub>d</sub>
</italic> for any accession (<xref ref-type="bibr" rid="B64">Yin and Johnson, 2000</xref>; <xref ref-type="bibr" rid="B20">Dyson et&#xa0;al., 2015</xref>), although this may be due to the difficulty in measuring dark respiration within the whole plant chamber. <italic>R<sub>d</sub>
</italic> is an essential component of light acclimation and normally rises and falls in line with <italic>P<sub>max</sub>
</italic>. A high <italic>R<sub>d</sub>
</italic> would be disadvantageous under low light periods.</p>
<p>
<xref ref-type="bibr" rid="B7">Bailey et&#xa0;al. (2001)</xref> used constant light to identify three distinct phases of acclimation in Ler; a low light response, a high light response and a less pronounced response at intermediate light intensities, which they linked to changes in the content and composition of the thylakoid components as well as both photosystems. This is consistent with the suggestion that the regulation of <italic>P<sub>max</sub>
</italic> and Chl <italic>a:b</italic> is largely independent (<xref ref-type="bibr" rid="B7">Bailey et&#xa0;al., 2001</xref>). Whilst acclimation to high light was also exhibited by Ws, the corresponding change in chlorophyll was not seen. However, a decrease in Chl <italic>a:b</italic> ratio under FL vs CL was also observed in the <italic>gpt</italic>2- mutants suggesting that the mutant was still able to acclimate to lower light intensities, but not higher intensities. It is unclear why the Ws background would show a different response to <italic>gpt</italic>2- when the <italic>P<sub>max</sub>
</italic> shows the typical response to HL. These findings suggest that the effect of fluctuating light on acclimation is to invoke multiple pathways that allow an acclimation response to both high and low irradiances.</p>
<p>
<xref ref-type="bibr" rid="B6">Athanasiou et&#xa0;al. (2010)</xref> grew plants outdoors in unheated green houses, and found that under naturally fluctuating light, WT Ws had a higher fitness relative to <italic>gpt</italic>2- mutants and WT Col. The same study also showed the inability for Col to dynamically acclimate to an increase in irradiance under controlled conditions (see <xref ref-type="supplementary-material" rid="SM1">
<bold>Supplementary Figure 1</bold>
</xref> in <xref ref-type="bibr" rid="B6">Athanasiou et&#xa0;al. (2010)</xref>). The fact that Col expresses GP T2 but does not acclimate (<xref ref-type="bibr" rid="B36">Niewiadomski et&#xa0;al., 2005</xref>) supports the hypothesis that alternative pathways, not involving GPT2, are necessary for dynamic acclimation under fluctuating light. The role of GPT2 is to translocate G6P into the chloroplast to enable starch synthesis (<xref ref-type="bibr" rid="B25">Kunz et&#xa0;al., 2010</xref>). This results in an increased chloroplastic phosphate pool, causing changes in gene expression enabling acclimation to high light. In contrast, <italic>gpt</italic>2- mutants have a higher photosynthesis rate at lower light levels than the parental WT Ws plants (<xref ref-type="bibr" rid="B20">Dyson et&#xa0;al., 2015</xref>). However, this improved photosynthetic rate may be a result of developmental acclimation, not dynamic. Nevertheless, combined with the significantly lower Chl <italic>a:b</italic> ratio found within this study, this suggests that acclimation components can operate independently.</p>
<p>So far we have taken a simplistic approach, focusing on antenna size as given by Chl <italic>a:b</italic> and features of the light response curve notably <italic>P<sub>max</sub>
</italic> which may be limited by Rubisco, stomatal conductance and electron transport rate depending on conditions. We may consider any component of the chloroplast to be part of acclimation and further work is needed to determine how these operate in relation to each other. For example, changes in Rubisco concentration and activity, along with molecular changes such as cytochrome-b/f activity and LHC and photosystem stoichiometry (<xref ref-type="bibr" rid="B32">Murchie and Horton, 1997</xref>; <xref ref-type="bibr" rid="B58">Walters et&#xa0;al., 1999</xref>; <xref ref-type="bibr" rid="B63">Yano and Terashima, 2001</xref>; <xref ref-type="bibr" rid="B57">Walters et&#xa0;al., 2004</xref>; <xref ref-type="bibr" rid="B50">Suorsa et&#xa0;al., 2012</xref>). We may determine some general trends, i.e., levels of Cytochrome-b/f, ATPase, plastoquinone and Rubisco will be needed to achieve high <italic>P<sub>max</sub>
</italic>, the question is how much. <xref ref-type="bibr" rid="B54">Vialet-Chabrand et&#xa0;al. (2017)</xref> showed that election transport was more important than Rubisco in <italic>Arabidopsis</italic> Col-0. There may be much variation in nature: there is evidence that in developmentally acclimated plants, some species do not change their chlorophyll <italic>a:b</italic> ratios (<xref ref-type="bibr" rid="B32">Murchie and Horton, 1997</xref>; <xref ref-type="bibr" rid="B65">Zivcak et&#xa0;al., 2014</xref>). Furthermore, some changes in chlorophyll <italic>a:b</italic> ratio have been attributed to genes involved in LHCII distribution, which is a known induction n response (<xref ref-type="bibr" rid="B2">Allen and Forsberg, 2001</xref>; <xref ref-type="bibr" rid="B18">Depge et&#xa0;al., 2003</xref>; <xref ref-type="bibr" rid="B8">Bellafiore et&#xa0;al., 2005</xref>; <xref ref-type="bibr" rid="B53">Vainonen et&#xa0;al., 2005</xref>; <xref ref-type="bibr" rid="B50">Suorsa et&#xa0;al., 2012</xref>; <xref ref-type="bibr" rid="B31">Mekala et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>).</p>
</sec>
<sec id="s4_2">
<label>4.2</label>
<title>&#x2018;Entrainment&#x2019; of photosynthetic capacity in fluctuating light is genotype - dependent</title>
<p>In previous work we formulated a mathematical framework of dynamic acclimation that defined the optimal adjustments to net photosynthesis under fluctuating light conditions (<xref ref-type="bibr" rid="B41">Retkute et&#xa0;al., 2015</xref>). Applied within this study we describe two key aspects of the acclimation process: first the rate of acclimation itself and second &#x2018;entrainment&#x2019; of <italic>P<sub>max</sub>
</italic> by the fluctuating light. As described previously, transient high light events induce a &#x2018;fading memory&#x2019; which influences both the induction state and the likelihood of inducing acclimation (<xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5</bold>
</xref>). We show a new feature of acclimation in fluctuating light which is the &#x2018;fading memory&#x2019; or &#x3c4; which varies according to genotype. This indicates that there is genetic variation for both speed of response to fluctuating light but also in the sensitivity to which the plants sense and measure light transients.</p>
<p>Previous research on variation among <italic>Arabidopsis</italic> accessions found variation between Ler-0 and Ws-2 in the PSI/PSII ratio, the lateral mobility of the thylakoid membrane and in chlorophyll protein complexes (<xref ref-type="bibr" rid="B24">Kaiser et&#xa0;al., 2020</xref>; <xref ref-type="bibr" rid="B61">W&#xf3;jtowicz and Gieczewska, 2021</xref>). In particular, the authors proposed that increased value of the nonphotochemical quenching qN or NPQ reported for Ler-0 under control conditions might limit the capacity for the photosynthetic apparatus to adapt to changing light intensities. NPQ is known to be sensitive to changes in the energy status of the chloroplasts (energy-dependent quenching) and thus presents the most sensitive parameter for the early detection of such changes. Whilst <xref ref-type="bibr" rid="B24">Kaiser et&#xa0;al. (2020)</xref> did not assess Ws, they found that certain photosynthetic traits were correlated with the ecological niche to which the accession originated. For example, they found that a reduction in PSII operating efficiency (<italic>&#x3d5;</italic>PSII) under fluctuating light correlates with latitude: with those originating further north exhibiting the lowest <italic>&#x3d5;</italic>PSII. Therefore our conclusion for variation in terms of the timing and rate of onset of acclimation is consistent with the known variation among <italic>Arabidopsis</italic> accessions.</p>
</sec>
<sec id="s4_3">
<label>4.3</label>
<title>Implication of photosynthetic acclimation for crop plants</title>
<p>Fluctuating light experiments have been performed on plants under natural conditions, these found that the ability to acclimate provided a fitness advantage by optimizing photosynthetic efficiency for a new environment (<xref ref-type="bibr" rid="B6">Athanasiou et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B50">Suorsa et&#xa0;al., 2012</xref>). However, in these experiments, plants were subject to fluctuations in temperature and humidity as well as light thus entangling photosynthetic acclimation to irradiance from that of temperature or humidity is difficult to achieve. Nevertheless, more realistic representations of the natural environment will be critical for determining the adaptive significance of acclimation and determining the limits placed on plants. However, quantifying the physiological response of plants under environmentally relevant conditions is extremely difficult (<xref ref-type="bibr" rid="B55">Walters, 2005</xref>).</p>
<p>Photosynthesis in nature responds largely to fluctuating light in addition to the fixed longer term square waves commonly used for studies in photoacclimation (<xref ref-type="bibr" rid="B39">Poorter et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B54">Vialet-Chabrand et&#xa0;al., 2017</xref>). Confounding this are species- and genotype-specific differences in plant structure as well as physiological capacity will influence the overall impact of growth conditions on performance (<xref ref-type="bibr" rid="B32">Murchie and Horton, 1997</xref>; <xref ref-type="bibr" rid="B6">Athanasiou et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B12">Burgess et&#xa0;al., 2017</xref>; <xref ref-type="bibr" rid="B9">Burgess et&#xa0;al., 2021</xref>). Acclimation is a complex process potentially involving most photosynthetic components in the chloroplast and experimental data indicates that the past light history of a leaf is critical in determining the optimal <italic>P<sub>max</sub>
</italic> under a given light level (e.g. <xref ref-type="fig" rid="f5">
<bold>Figure&#xa0;5</bold>
</xref>; <xref ref-type="bibr" rid="B41">Retkute et&#xa0;al. (2015)</xref>). Whilst this can be controlled or determined relatively easily within small plants with simple structures, such as <italic>Arabidopsis</italic>, knowledge of the past light history is difficult to obtain for larger plants, or crop plants, like rice (<italic>Oryza sativa</italic>) and wheat (<italic>Triticum aestivum</italic>) (<xref ref-type="bibr" rid="B33">Murchie et&#xa0;al., 2002</xref>; <xref ref-type="bibr" rid="B35">Murchie et&#xa0;al., 2008</xref>; <xref ref-type="bibr" rid="B52">Townsend et&#xa0;al., 2018</xref>; <xref ref-type="bibr" rid="B9">Burgess et&#xa0;al., 2021</xref>). The complex canopy structure of these plants combined with environmental factors such as weather conditions and wind, cloud or solar movement mean that a given section of leaf within the same plant will be subject to light changes that vary in frequency and longevity (<xref ref-type="bibr" rid="B11">Burgess et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B12">Burgess et&#xa0;al., 2017</xref>; <xref ref-type="bibr" rid="B9">Burgess et&#xa0;al., 2021</xref>). Knowledge of the underlying mechanisms of this process, what fitness advantages acclimation provides and how it could be manipulated will therefore be critical in targeting crops for improved productivity and yield.</p>
</sec>
</sec>
<sec id="s5">
<label>5</label>
<title>Concluding remarks</title>
<p>In consensus with the literature, our findings suggest that dynamic acclimation to high- and low light are controlled by at least two distinct mechanisms, and that both are utilized in <italic>A. thaliana</italic>. Whilst <italic>GPT</italic>2 is required for high light acclimation, it does not seem to be necessary for low light acclimation. Furthermore, whilst light history influences the capacity to acclimate to a change in irradiance, the length, or speed, of response to light history is also genotype specific. This lays the necessary groundwork for understanding the features of fluctuating light and the speed and direction of multi-faceted responses that provide optimal acclimation state to both high and low light within short time periods.</p>
</sec>
<sec id="s6" sec-type="data-availability">
<title>Data availability statement</title>
<p>The raw data supporting the conclusions of this article will be made available by the authors, without undue reservation.</p>
</sec>
<sec id="s7" sec-type="author-contributions">
<title>Author contributions</title>
<p>All authors conceived the project. AB performed the physical experimentation whilst RR performed the modelling analysis. RR and AB wrote the article with input from EM. All authors contributed to the article and approved the submitted version.</p>
</sec>
</body>
<back>
<sec id="s8" sec-type="funding-information">
<title>Funding</title>
<p>AB is supported by the Leverhulme Trust as an Early Career Fellow. This work was supported by the UKRI Molecules to Landscapes call [grant number BB/X00595X/1].</p>
</sec>
<ack>
<title>Acknowledgments</title>
<p>The authors wish to acknowledge Professor Giles Johnson for access to the <italic>gpt2-</italic> mutant seed used within this study and to Conor Simpson for assistance in physical measurements.</p>
</ack>
<sec id="s9" sec-type="COI-statement">
<title>Conflict of interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec id="s10" sec-type="disclaimer">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
<sec id="s11" sec-type="supplementary-material">
<title>Supplementary material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/fpls.2023.1116367/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fpls.2023.1116367/full#supplementary-material</ext-link>
</p>
<supplementary-material xlink:href="Image_1.jpg" id="SM1" mimetype="image/jpeg"/>
</sec>
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