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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.2021.768963</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>Extending the Cultivation Area of Pecan (<italic>Carya illinoinensis</italic>) Toward the South in Southeastern Subtropical China May Cause Increased Cold Damage</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name><surname>Zheng</surname> <given-names>Jinbin</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="author-notes" rid="fn002"><sup>&#x2020;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/1513821/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>H&#x00E4;nninen</surname> <given-names>Heikki</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<xref ref-type="author-notes" rid="fn002"><sup>&#x2020;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/100901/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Lin</surname> <given-names>Jianhong</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="author-notes" rid="fn003"><sup>&#x2021;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/1560042/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Shen</surname> <given-names>Sitian</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="author-notes" rid="fn003"><sup>&#x2021;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/1560046/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name><surname>Zhang</surname> <given-names>Rui</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<xref ref-type="corresp" rid="c001"><sup>&#x002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/1462944/overview"/>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>State Key Laboratory of Subtropical Silviculture, Zhejiang A&#x0026;F University</institution>, <addr-line>Hangzhou</addr-line>, <country>China</country></aff>
<aff id="aff2"><sup>2</sup><institution>SFGA Research Center for Torreya Grandis, Zhejiang A&#x0026;F University</institution>, <addr-line>Hangzhou</addr-line>, <country>China</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Yann Vitasse, Swiss Federal Institute for Forest, Snow and Landscape Research (WSL), Switzerland</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: B&#x00E9;n&#x00E9;dicte Wenden, Institut National de la Recherche Agronomique (INRA), France; Catherine Chamberlain, Conservation International, United States</p></fn>
<corresp id="c001">&#x002A;Correspondence: Rui Zhang, <email>rui.zhang@zafu.edu.cn</email></corresp>
<fn fn-type="equal" id="fn002"><p><sup>&#x2020;</sup>These authors have contributed equally to this work</p></fn>
<fn fn-type="present-address" id="fn003"><p><sup>&#x2021;</sup>Present address: Jianhong Lin, CNRS, AgroParisTech, Ecologie Syst&#x00E9;matique et Evolution, Universit&#x00E9; Paris-Saclay, Orsay, France Sitian Shen, School of GeoSciences, University of Edinburgh, Edinburgh, United Kingdom</p></fn>
<fn fn-type="other" id="fn004"><p>This article was submitted to Functional Plant Ecology, a section of the journal Frontiers in Plant Science</p></fn>
</author-notes>
<pub-date pub-type="epub">
<day>30</day>
<month>11</month>
<year>2021</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>12</volume>
<elocation-id>768963</elocation-id>
<history>
<date date-type="received">
<day>01</day>
<month>09</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>02</day>
<month>11</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x00A9; 2021 Zheng, H&#x00E4;nninen, Lin, Shen and Zhang.</copyright-statement>
<copyright-year>2021</copyright-year>
<copyright-holder>Zheng, H&#x00E4;nninen, Lin, Shen and Zhang</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>Pecan (<italic>Carya illinoinensis</italic>) is an important nut tree species in its native areas in temperate and subtropical North America, and as an introduced crop in subtropical southeastern China as well. We used process-based modeling to assess the effects of climatic warming in southeastern China on the leaf-out phenology of pecan seedlings and the subsequent risk of &#x201C;false springs,&#x201D; i.e., damage caused by low temperatures occurring as a result of prematurely leafing out. In order to maximize the biological realism of the model used in scenario simulations, we developed the model on the basis of experiments explicitly designed for determining the responses modeled. The model showed reasonable internal accuracy when calibrated against leaf-out observations in a whole-tree chamber (WTC) experiment with nine different natural-like fluctuating temperature treatments. The model was used to project the timing of leaf-out in the period 2022&#x2013;2099 under the warming scenarios RCP4.5 and RCP8.5 in southeastern China. Two locations in the main pecan cultivation area in the northern subtropical zone and one location south of the main cultivation area were addressed. Generally, an advancing trend of leaf-out was projected for all the three locations under both warming scenarios, but in the southern location, a delay was projected under RCP8.5 in many years during the first decades of the 21st century. In the two northern locations, cold damage caused by false springs was projected to occur once in 15&#x2013;26 years at most, suggesting that pecan cultivation can be continued relatively safely in these two locations. Paradoxically, more frequent cold damage was projected for the southern location than for the two northern locations. The results for the southern location also differed from those for the northern locations in that more frequent cold damage was projected under the RCP4.5 warming scenario (once in 6 years) than under the RCP8.5 scenario (once in 11 years) in the southern location. Due to the uncertainties of the model applied, our conclusions need to be re-examined in an additional experimental study and further model development based on it; but on the basis of our present results, we do not recommend starting large-scale pecan cultivation in locations south of the present main pecan cultivation area in southeastern subtropical China.</p>
</abstract>
<kwd-group>
<kwd>chilling requirement</kwd>
<kwd>climatic warming</kwd>
<kwd>experimental ecophysiology</kwd>
<kwd>leaf-out</kwd>
<kwd>pecan</kwd>
<kwd>process-based tree phenology models</kwd>
<kwd>scenario simulations</kwd>
<kwd>subtropical trees</kwd>
</kwd-group>
<contract-num rid="cn001">32171832; 31800579</contract-num>
<contract-sponsor id="cn001">National Natural Science Foundation of China<named-content content-type="fundref-id">10.13039/501100001809</named-content></contract-sponsor>
<counts>
<fig-count count="7"/>
<table-count count="2"/>
<equation-count count="14"/>
<ref-count count="72"/>
<page-count count="16"/>
<word-count count="13809"/>
</counts>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="S1">
<title>Introduction</title>
<p>The timing of phenological events of trees in spring, such as leafing out of vegetative buds, is crucial for the survival and growth of trees (<xref ref-type="bibr" rid="B24">Fuchigami et al., 1982</xref>; <xref ref-type="bibr" rid="B29">H&#x00E4;nninen, 2016</xref>; <xref ref-type="bibr" rid="B51">Perez-de-Lis et al., 2016</xref>). At the ecosystem level, the spring phenology of trees regulates several key processes, such as the cycling of carbon and nutrients and productivity of forests and plantations (<xref ref-type="bibr" rid="B52">Piao et al., 2009</xref>; <xref ref-type="bibr" rid="B35">Keenan et al., 2014</xref>; <xref ref-type="bibr" rid="B71">Zhou et al., 2020</xref>). In the temperate zone, analyses of long-term phenological records have shown a general advancement of spring phenology over the past few decades caused by global warming (<xref ref-type="bibr" rid="B55">Richardson et al., 2013</xref>; <xref ref-type="bibr" rid="B63">Vitasse et al., 2018</xref>). However, several cases have also been found where the advancement has been leveling off (<xref ref-type="bibr" rid="B23">Fu et al., 2015</xref>).</p>
<p>Air temperature is a major environmental factor regulating the spring phenology of trees in boreal and temperate zones. It has a dual role (<xref ref-type="bibr" rid="B56">Sarvas, 1972</xref>, <xref ref-type="bibr" rid="B57">1974</xref>; <xref ref-type="bibr" rid="B53">Polgar and Primack, 2011</xref>). First, after growth cessation and bud set in the autumn, long-term exposure to chilling temperatures is required for a rest break, synonymous to endodormancy release (<xref ref-type="bibr" rid="B38">Lang et al., 1987</xref>), which means the removal of growth-arresting physiological conditions within the buds (<xref ref-type="bibr" rid="B24">Fuchigami et al., 1982</xref>; <xref ref-type="bibr" rid="B17">Cooke et al., 2012</xref>; <xref ref-type="bibr" rid="B31">H&#x00E4;nninen et al., 2019</xref>). Temperatures in the range of 0&#x2013;10&#x00B0;C have traditionally been regarded as the most effective in causing rest breaks (<xref ref-type="bibr" rid="B57">Sarvas, 1974</xref>; <xref ref-type="bibr" rid="B29">H&#x00E4;nninen, 2016</xref>). Second, after the chilling requirement of rest completion is met, the period of quiescence, synonymous with ecodormancy (<xref ref-type="bibr" rid="B38">Lang et al., 1987</xref>), is attained. In quiescence, bud burst is prevented only by environmental factors, typically low air temperatures, so that it takes prolonged exposure to relatively high forcing temperatures to cause the occurrence of visible phenological events, such as leafing out and flowering (<xref ref-type="bibr" rid="B56">Sarvas, 1972</xref>, <xref ref-type="bibr" rid="B57">1974</xref>). Besides air temperature, photoperiod has long been considered to regulate the spring phenology of trees, at least in some species (<xref ref-type="bibr" rid="B65">Wareing, 1953</xref>; <xref ref-type="bibr" rid="B4">Caffarra and Donnelly, 2011</xref>; <xref ref-type="bibr" rid="B61">Vitasse and Basler, 2013</xref>); more recently, further evidence for the role of photoperiod has been published (<xref ref-type="bibr" rid="B2">Basler and K&#x00F6;rner, 2012</xref>; <xref ref-type="bibr" rid="B22">Fu et al., 2019</xref>; <xref ref-type="bibr" rid="B47">Meng et al., 2021</xref>).</p>
<p>The past few decades have seen a growing trend of constructing process-based models of the spring phenology of boreal and temperate trees. These models address the developmental phenomena taking place during periods of rest and quiescence with explicit state variables (<xref ref-type="bibr" rid="B29">H&#x00E4;nninen, 2016</xref>; <xref ref-type="bibr" rid="B16">Chuine and R&#x00E9;gni&#x00E8;re, 2017</xref>). Recently, it has been shown experimentally that subtropical trees also show a rest period and chilling requirement (<xref ref-type="bibr" rid="B19">Du et al., 2019</xref>; <xref ref-type="bibr" rid="B58">Song et al., 2020</xref>; <xref ref-type="bibr" rid="B33">Jewaria et al., 2021</xref>; <xref ref-type="bibr" rid="B50">Pan et al., 2021</xref>; <xref ref-type="bibr" rid="B67">Zhang et al., 2021a</xref>, <xref ref-type="bibr" rid="B68">b</xref>). The first process-based models of spring phenology have been published for subtropical trees (<xref ref-type="bibr" rid="B13">Chen et al., 2017</xref>; <xref ref-type="bibr" rid="B69">Zhang et al., 2021c</xref>).</p>
<p>Since the 1980s, process-based models of the spring phenology of trees have been applied to project the effects of climatic warming on boreal and temperate trees (<xref ref-type="bibr" rid="B9">Cannell, 1985</xref>; <xref ref-type="bibr" rid="B27">H&#x00E4;nninen, 1991</xref>; <xref ref-type="bibr" rid="B62">Vitasse et al., 2011</xref>; <xref ref-type="bibr" rid="B14">Chuine et al., 2016</xref>; <xref ref-type="bibr" rid="B21">Ford et al., 2016</xref>; <xref ref-type="bibr" rid="B64">Wang et al., 2020</xref>). Climatic warming may have two different adverse effects on the spring phenology of trees. First, especially under warm climates, reduced chilling under climatic warming may delay the spring leaf-out and flowering (<xref ref-type="bibr" rid="B48">Murray et al., 1989</xref>), and the warming may even cause abnormal development of vegetative and flower buds in the most severe cases, thus reducing the growth and production of fruits (<xref ref-type="bibr" rid="B20">Erez, 2000</xref>; <xref ref-type="bibr" rid="B44">Man et al., 2017</xref>). Second, warming may advance the spring leaf-out and flowering to the extent that the risk of damage caused by low spring temperatures increases (<xref ref-type="bibr" rid="B9">Cannell, 1985</xref>; <xref ref-type="bibr" rid="B27">H&#x00E4;nninen, 1991</xref>). This phenomenon, more recently called &#x201C;false spring&#x201D; (<xref ref-type="bibr" rid="B45">Marino et al., 2011</xref>; <xref ref-type="bibr" rid="B11">Chamberlain et al., 2019</xref>), may cause considerable damage even under the present climate (<xref ref-type="bibr" rid="B25">Gu et al., 2008</xref>; <xref ref-type="bibr" rid="B34">Kaur et al., 2020</xref>). However, if the advancement of spring phenology is not accompanied by the increased incidence of cold damage, then climatic warming may increase the productivity of trees and forests by prolonging the growing season (<xref ref-type="bibr" rid="B37">Kramer and H&#x00E4;nninen, 2009</xref>). In all, trustworthy projection of the effects of warming on the spring phenology of trees calls for biologically realistic process-based models.</p>
<p>Pecan (<italic>Carya illinoinensis</italic>) was introduced to China about a 100 years ago from the United States, where it has a broad geographical range in both the temperate and subtropical zones. Now it is a major horticultural crop in subtropical southeastern China (<xref ref-type="bibr" rid="B70">Zhang et al., 2015</xref>). <xref ref-type="bibr" rid="B59">Sparks (1993)</xref> showed that pecan evinces a rest period and a chilling requirement of a rest break. Here, we developed a process-based model for spring leaf-out in seedlings of pecan grown in southeastern subtropical China. We took an experimental approach, where model development was based on growth chamber experiments explicitly designed to examine the processes addressed by the models. The model developed was applied to project the timing of pecan seedling leaf-out and the subsequent risk of cold damage under two climatic scenarios. In the simulations, we examined which one of the three hypotheses was projected to be realized in pecan seedlings grown in three locations in southeastern China: (1) leaf-out is delayed as a result of reduced chilling (the delay hypothesis), (2) leaf-out is advanced to the extent of causing the increased occurrence of cold damage (the false spring hypothesis), and (3) leaf-out is advanced without increased incidence of cold damage (the prolonged growing season hypothesis).</p>
</sec>
<sec id="S2" sec-type="materials|methods">
<title>Materials and Methods</title>
<sec id="S2.SS1">
<title>Structure of the Overall Model</title>
<p>The process-based spring phenology model for pecan leaf-out was developed by applying a modular model structure consisting of three sub-models (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1</xref>; <xref ref-type="bibr" rid="B26">H&#x00E4;nninen, 1990</xref>, <xref ref-type="bibr" rid="B29">2016</xref>; <xref ref-type="bibr" rid="B30">H&#x00E4;nninen and Kramer, 2007</xref>; for recent applications of the approach, refer to <xref ref-type="bibr" rid="B43">Lundell et al., 2020</xref>; <xref ref-type="bibr" rid="B69">Zhang et al., 2021c</xref>). Sub-models I and II correspond to the various chilling and forcing accumulation models (<xref ref-type="bibr" rid="B36">Kramer, 1994</xref>; <xref ref-type="bibr" rid="B15">Chuine et al., 1998</xref>), respectively, but in order to emphasize the physiological phenomena modeled, we use the biological names of the rate and state variables here (<xref ref-type="bibr" rid="B28">H&#x00E4;nninen, 1995</xref>, <xref ref-type="bibr" rid="B29">2016</xref>; <xref ref-type="bibr" rid="B31">H&#x00E4;nninen et al., 2019</xref>; <xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1</xref>).</p>
<p>Sub-model I addresses the effects of the chilling temperatures on the rate of a rest break, R<sub>t</sub>(t) (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1</xref>). The state of rest break, S<sub>r</sub>(t), is obtained by integrating R<sub>r</sub>(t) with respect to time from the onset of rest, t<sub>0</sub>, to time instant t. R<sub>t</sub>(t) is scaled on a percentage scale, so that rest completion is predicted to take place when S<sub>t</sub>(t) = 100%. Sub-model II addresses the ontogenetic development, i.e., the microscopic anatomical changes within the bud that lead to the visible phenological event, such as leafing out. In particular, Sub-model II addresses the effects of high forcing temperatures on the potential rate of ontogenetic development, R<sub>o,pot</sub>(t) (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1</xref>). The potential rate indicates the rate after rest completion when the rate is no longer restricted by the rest status of the bud.</p>
<p>The restrictions caused by the rest status are addressed by sub-model III, where the value of a theoretical variable, ontogenetic competence, C<sub>o</sub>(t), is calculated as a function of the state of rest break, S<sub>r</sub>(t). C<sub>o</sub> is a [0,1]-multiplier mediating the effects of rest status to the (realized) rate of ontogenetic development, R<sub>o</sub>(t) (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1</xref>). With C<sub>o</sub>(t) = 0, no ontogenetic development takes place regardless of the ambient temperature. At rest completion with R<sub>t</sub>(t) = 100%, the value ontogenetic competence is C<sub>o</sub>(t) = 1 by definition. Otherwise, the relationship between C<sub>o</sub>(t) and S<sub>r</sub>(t) can take different forms, making it possible to address contrasting models, such as the parallel model and the sequential model, within the same framework (<xref ref-type="bibr" rid="B26">H&#x00E4;nninen, 1990</xref>, <xref ref-type="bibr" rid="B29">2016</xref>). Finally, the state of ontogenetic development, S<sub>o</sub>(t), is obtained by integrating R<sub>r</sub>(t) with respect to time from the onset of rest, t<sub>0</sub>, to time instant t. Leaf-out is predicted to occur when S<sub>o</sub>(t) = 100%.</p>
</sec>
<sec id="S2.SS2">
<title>Experimental Designs and Conditions</title>
<sec id="S2.SS2.SSS1">
<title>Autumn Experiment</title>
<p>In the autumn experiment, the effects of chilling on rest break and, further, on ontogenetic competence were examined (sub-models I and III, <xref ref-type="supplementary-material" rid="DS1">Supplementary Figures 1</xref>, <xref ref-type="supplementary-material" rid="DS1">2</xref>). The experimental seedlings were first exposed to chilling for periods of varying duration, either under natural conditions outdoors or under controlled conditions in growth chambers, and then transferred to high-temperature forcing conditions in growth chambers. In the latter, a regrowth test was carried out by observing the occurrence and timing of leaf-out (for details, refer to <xref ref-type="supplementary-material" rid="DS1">Supplementary Material</xref>). The controlled chilling treatment was carried out for the purpose of formulating sub-models I and III (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1</xref>). The natural chilling treatment was carried out to determine the timing of rest completion under natural conditions. This information was used to determine the timing of the spring experiment, whose results were used in formulating sub-model II.</p>
<p>The controlled chilling took place in computer-controlled growth chambers (E-Lotus Technology Co., Beijing, China): air temperature +6&#x00B0;C, constant day length 10 h 30 min, with the light period from 6:30 am to 5 pm, and a relatively low photosynthetic photon flux density (PPFD) (150 &#x03BC;mol m<sup>&#x2013;2</sup> s<sup>&#x2013;1</sup>). The conditions in the controlled chilling approximated those typical for the winter months in the area. Two chilling chambers (2.55 m &#x00D7; 2 m &#x00D7; 2.5 m) were used in the experiment. Both chambers had eight shelves (0.6 m &#x00D7; 1.1 m) with LED lights located above the shelves. The forcing took place in computer-controlled growth chambers (E-Lotus Technology Co., Beijing, China): air temperature +20&#x00B0;C, constant day length 12 h, with the light period from 6.30 am to 6.30 pm, and a relatively high PPFD (400 &#x03BC;mol m<sup>&#x2013;2</sup> s<sup>&#x2013;1</sup>). The conditions in the forcing chambers approximated those prevailing in the area at the spring equinox, some weeks before the leaf-out of most tree species is observed under natural conditions. Two forcing chambers (4.92 m &#x00D7; 2 m &#x00D7; 2.5 m) were also used in the study. Both chambers had four shelves (0.6 m &#x00D7; 2.3 m) with LED lights located above the shelves. In both the chilling and the forcing chambers, the relative humidity was 70&#x2013;80%, concentration was CO<sub>2</sub> 300&#x2013;400 ppm, and air circulation was carried out four times a day for 20 min each time. The seedlings were watered every 3 days in the chilling chambers and every 2 days in the forcing chambers.</p>
<p>At the beginning of the experiment, on November 21, 2017, 10 seedlings were sampled from the outdoor seedling collection for the forcing conditions (0 weeks chilling). Out of the remaining 120 seedlings, one-half were sampled for controlled chilling in the growth chambers, while the other half remained under natural chilling conditions outdoors. After that, 10 seedlings from both chilling conditions were sampled at 2-week intervals for the forcing conditions. The last transfer was carried out on February 12, 2018, so the duration of chilling varied from 0 to 84 days. Under the forcing conditions, leaf-out was inspected at intervals of 2 or 3 days (for details, refer to <xref ref-type="supplementary-material" rid="DS1">Supplementary Material</xref>). The leaf-out observations under the forcing conditions were stopped on April 23, 2018.</p>
<p>In the analysis of the results, the generic term &#x201C;bud burst&#x201D; was used for leaf-out (<xref ref-type="bibr" rid="B67">Zhang et al., 2021a</xref>). This was done in order to report the results in terms of standard indices bud burst percentage, BB%, and days to bud burst, DBB. Accordingly, for each treatment group, defined by the duration (0&#x2013;84 days) and type (natural, controlled) of chilling, BB% was calculated as the percentage of seedlings showing leaf-out. Additionally, for each seedling showing leaf-out, DBB was determined as the time required under the forcing conditions for leaf-out. In the analysis of the results, both BB% and DBB were plotted against the duration of chilling.</p>
</sec>
<sec id="S2.SS2.SSS2">
<title>Spring Experiment</title>
<p>In the spring experiment, the effects of relatively high air temperatures (&#x201C;forcing&#x201D;) on the timing of leaf-out were examined (sub-model II; <xref ref-type="supplementary-material" rid="DS1">Supplementary Figures 1</xref>, <xref ref-type="supplementary-material" rid="DS1">2</xref>). After overwintering under natural conditions, 10 seedlings were sampled from the natural outdoor conditions for each of the three growth chambers (E-Lotus Technology Co., Beijing, China) with constant air temperatures of +10, +17, and +24&#x00B0;C. The environmental conditions other than air temperature were the same as in the autumn experiment: 12-h day length, PPFD 400 &#x03BC;mol m<sup>&#x2013;2</sup> s<sup>&#x2013;1</sup>, relative humidity 70&#x2013;80%, and concentration of CO<sub>2</sub> 300&#x2013;400 ppm. Leaf-out was observed in each chamber every 3 days. The days to bud burst (leaf-out), DBB, was recorded for each experimental seedling, and in the analysis of the results, the observations were plotted against the experimental temperature. The data were used for formulating sub-model II (air temperature response of the potential rate of ontogenetic development). For such a purpose, the experiment should optimally be started after rest is completed, but there should be no occurrence of considerable ontogenetic development caused by high temperatures under natural conditions. If such ontogenetic development had already occurred under the natural conditions before the start of the experiment, that would decrease the value of DBB and, thereby produce erroneous data for the modeling. This optimal timing was not known <italic>a priori</italic>, which is why the experiment was repeated at three different times by transferring a sample of the seedlings from the natural outdoor conditions to the three growth chambers each time. The transfer dates were February 13, 2017, February 27, 2017, and March 13, 2018. For independent model testing, leaf-out was additionally observed in a control group of 10 seedlings that remained under natural conditions throughout the experiment.</p>
</sec>
<sec id="S2.SS2.SSS3">
<title>Whole-Tree Chamber Experiment</title>
<p>In the whole-tree (WTC) experiment, the effects of autumn, winter, and spring temperatures on the timing of leaf-out were examined under conditions similar to those occurring naturally. All the treatments were based on the natural ambient temperature, and natural photoperiod was applied (for details, refer to below). The results of the WTC experiment were used for estimating the parameters t<sub>0</sub> and T<sub>upp</sub> (refer to the section &#x201C;Constructing the sub-models on the basis of experimental data&#x201D; below) and for testing the accuracy of the overall model (internal validation) (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 2</xref>).</p>
<p>Three temperature levels were included: ambient, ambient +2&#x00B0;C, and ambient +4&#x00B0;C. The experiment was started on November 10, 2019, and for the definition of our treatments, we denoted &#x201C;winter&#x201D; as the period of November 10, 2019, to February 10, 2020. The time after that, until the observed leaf-out, was denoted as &#x201C;spring.&#x201D; A factorial 3 &#x00D7; 3 design was adopted for the experiment, such that each of the three levels of winter temperature was combined with the corresponding three levels of spring temperature, thus creating a total of nine treatments (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 2</xref>). In each treatment, there were eight replicated seedlings.</p>
<p>The experiment was implemented with three transparent whole-tree chambers (WTCs, E-Lotus Technology Co., Beijing, China). The chambers have a smart temperature control system to keep the temperature at the intended level. In one chamber, the air temperature was kept at the ambient level. In the other two WTCs, the air temperature was elevated by 2 and 4&#x00B0;C, respectively, above the ambient temperature. The experiment was implemented by (1) placing the seedlings of each treatment group in the chamber representing the intended winter temperature at the beginning of the experiment, and (2) transferring the seedlings on February 11, 2020, to the intended spring temperature (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 2</xref>). In order to avoid any systematic errors caused by possible temperature gradients within the chambers, the locations of the seedlings in the chambers were rotated constantly during the experiment.</p>
</sec>
</sec>
<sec id="S2.SS3">
<title>Statistical Analysis of the Experimental Results</title>
<p>In the autumn experiment, the differences in BB% between the treatments were analyzed by means of logistic regression with a binary response (bud burst: no/yes) using the type (natural vs. controlled in +6&#x00B0;C) and duration of chilling as the explaining factors. The differences in DBB between the treatments were analyzed by means of a two-way ANOVA using the same explaining factors as with BB%. A two-way ANOVA was also applied to analyze the differences in DBB between the treatments in the spring experiment. The explaining factors were the time of transfer from natural conditions to forcing conditions and the temperature under the forcing conditions.</p>
</sec>
<sec id="S2.SS4">
<title>Constructing the Sub-Models on the Basis of Experimental Data</title>
<sec id="S2.SS4.SSS1">
<title>A Framework for Formulating the Models on the Basis of Experimental Data</title>
<p>The three sub-models were constructed on the basis of experimental data, following the methodological framework introduced by <xref ref-type="bibr" rid="B69">Zhang et al. (2021c)</xref>, with few modifications. The air temperature responses described by the three sub-models were inferred on the basis of their implications for the responses to the occurrence and timing of the readily observable leaf-out under the experimental conditions. Because of these peculiarities of the phenomena modeled, the use of experimental data involved two steps: first, the empirical data points were calculated by analyzing the experimental leaf-out data. Second, the data points were plotted against the respective explanatory variable, and a response curve was fitted to the data.</p>
</sec>
<sec id="S2.SS4.SSS2">
<title>Sub-Model I</title>
<p>For any constant temperature T&#x2032;, the empirical value of the rate of rest break was calculated as (<xref ref-type="bibr" rid="B57">Sarvas, 1974</xref>; <xref ref-type="bibr" rid="B69">Zhang et al., 2021c</xref>)</p>
<disp-formula id="S3.E1"><label>(1)</label><mml:math id="M1" display="block"><mml:mrow><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi>r</mml:mi></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msup><mml:mi>T</mml:mi><mml:mo>&#x2032;</mml:mo></mml:msup><mml:mo rspace="5.8pt">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:mrow><mml:mn>100</mml:mn><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mi>t</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:mrow></mml:mfrac></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>where, &#x0394;t = the duration of chilling required for rest completion in the autumn experiment. As a result of using the multiplier 100, the scale for the rest break is the percentage scale [0,100%], so the value of R<sub>r</sub> calculated with Equation (1) indicates the percentage, out of the total number of physiological reactions required for rest completion, of such reactions taking place in 1 h. The value of &#x0394;t was determined in terms of days at first but then converted to hours by multiplying the original value by 24 because the model was applied with a time step of 1 h.</p>
<p>The requirement set for rest completion was that in the regrowth test under forcing conditions the bud burst (leaf-out) percentage, BB%, is at or near 100% and that the curve representing days to bud burst (leaf-out), DBB, as a function of the duration of chilling levels off, indicating that the rate of ontogenetic development cannot be substantially increased by further chilling. Following <xref ref-type="bibr" rid="B69">Zhang et al. (2021c)</xref>, we determined &#x0394;t for the controlled chilling treatment in +6&#x00B0;C by requiring that the BB% is at least 80% and by determining the leveling off of the DBB curve as follows: first, an exponential curve was fitted to the scatter plot representing the DBB of each of the seedlings as a function of the duration of chilling:</p>
<disp-formula id="S3.E2"><label>(2)</label><mml:math id="M2" display="block"><mml:mrow><mml:mrow><mml:mtext>y</mml:mtext><mml:mrow><mml:mo>(</mml:mo><mml:mtext>x</mml:mtext><mml:mo rspace="5.8pt">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mtext>x</mml:mtext><mml:mo rspace="5.8pt">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mn>0</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:msup><mml:mtext>e</mml:mtext><mml:mrow><mml:mo>-</mml:mo><mml:mrow><mml:msub><mml:mi>b</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mrow><mml:mtext>x</mml:mtext></mml:mrow></mml:mrow></mml:mrow></mml:msup></mml:mrow></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>where, y = the modeled value of days to bud burst; x = the duration of chilling (days); and y<sub>o</sub>, a<sub>1</sub>, and b<sub>1</sub> are parameters to be estimated. Then, in order to study the slope of the DBB curve, its first derivative with respect to the duration of chilling, x, was calculated as follows:</p>
<disp-formula id="S3.E3"><label>(3)</label><mml:math id="M3" display="block"><mml:mrow><mml:mpadded width="+3.3pt"><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mpadded><mml:mo>=</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:msub><mml:mi>b</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mrow><mml:msub><mml:mi>b</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mi>x</mml:mi></mml:mrow></mml:mrow></mml:msup></mml:mrow></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>Following <xref ref-type="bibr" rid="B69">Zhang et al. (2021c)</xref>, we determined &#x0394;t as equal to the duration of chilling x, where the value of the first derivative is equal to &#x2212;0.3 (refer to <xref ref-type="fig" rid="F1">Figure 1C</xref> in the section &#x201C;Results&#x201D;):</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption><p>Effects of chilling on a rest break in first-year pecan seedlings in the autumn experiment, where both controlled chilling in constant +6&#x00B0;C <bold>(A,C)</bold> and chilling outdoors under natural conditions <bold>(B,D)</bold> were used. The rest break caused by prolonged chilling is manifested after the transfer to the growth-promoting forcing conditions as an increase in panels <bold>(A,B)</bold> bud burst percentage, BB% and a decrease in panels <bold>(C,D)</bold> days to bud burst (DBB). The arrow and the index &#x0394;t indicate the estimated number of days required for meeting the chilling requirement of rest completion under the chilling conditions. The black dot indicates the corresponding value of the DBB at the time of rest completion. Note that the phenological event observed was leaf-out but that the concept &#x201C;bud burst&#x201D; is used here as a generic one facilitating the use of the standard indices BB% and DBB.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-12-768963-g001.tif"/>
</fig>
<disp-formula id="S3.E4"><label>(4)</label><mml:math id="M4" display="block"><mml:mrow><mml:mpadded width="+3.3pt"><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mpadded><mml:mo>=</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:msub><mml:mi>b</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mpadded width="+3.3pt"><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mrow><mml:msub><mml:mi>b</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mi>x</mml:mi></mml:mrow></mml:mrow></mml:msup></mml:mpadded></mml:mrow></mml:mrow><mml:mo>=</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.3</mml:mn></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>implying</p>
<disp-formula id="S3.E5"><label>(5)</label><mml:math id="M5" display="block"><mml:mrow><mml:mrow><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mpadded width="+3.3pt"><mml:mtext>t</mml:mtext></mml:mpadded></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:mpadded width="+3.3pt"><mml:mtext>x</mml:mtext></mml:mpadded><mml:mo rspace="5.8pt">=</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mrow><mml:mfrac><mml:mn>1</mml:mn><mml:msub><mml:mi>b</mml:mi><mml:mn>1</mml:mn></mml:msub></mml:mfrac><mml:mrow><mml:mi>ln</mml:mi><mml:mo>&#x2061;</mml:mo><mml:mfrac><mml:mn>0.3</mml:mn><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:msub><mml:mi>b</mml:mi><mml:mn>1</mml:mn></mml:msub></mml:mrow></mml:mfrac></mml:mrow></mml:mrow></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>Finally, the empirical value of the rate of rest break in +6&#x00B0;C was calculated by plugging the value of &#x0394;t obtained with Equation (5) for that treatment into Equation (1).</p>
<p>Due to the limited growth chamber facilities, we were not able to include other controlled constant chilling temperatures beside the +6&#x00B0;C used in the study. In the absence of experimental data for other temperatures, we determined sub-model I as follows (<xref ref-type="bibr" rid="B43">Lundell et al., 2020</xref>): (1) a plateau temperature response in the temperature range from the lower threshold temperature of &#x2212;3.4&#x00B0;C (<xref ref-type="bibr" rid="B57">Sarvas, 1974</xref>) to the upper threshold temperature, T<sub>upp</sub>, and (2) no rest break taking place below the lower or above the upper threshold (refer to <xref ref-type="fig" rid="F3">Figure 3A</xref> in the section &#x201C;Results&#x201D;):</p>
<disp-formula id="S3.E11"><mml:math id="M11" display="block"><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi>r</mml:mi></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo rspace="5.8pt">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:mn>0</mml:mn></mml:mrow><mml:mo rspace="7.5pt">,</mml:mo><mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mi>h</mml:mi><mml:mi>e</mml:mi><mml:mpadded width="+5pt"><mml:mi>n</mml:mi></mml:mpadded><mml:mi>T</mml:mi></mml:mrow><mml:mo>&lt;</mml:mo><mml:mrow><mml:mo>-</mml:mo><mml:mrow><mml:msup><mml:mn>3.4</mml:mn><mml:mo>&#x00B0;</mml:mo></mml:msup><mml:mtext>C</mml:mtext></mml:mrow></mml:mrow></mml:mrow></mml:mrow></mml:math></disp-formula>
<disp-formula id="S3.E12"><mml:math id="M12" display="block"><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi>r</mml:mi></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo rspace="5.8pt">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mrow><mml:mi>o</mml:mi><mml:mi>b</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:mrow></mml:msub></mml:mrow><mml:mo rspace="7.5pt">,</mml:mo><mml:mrow><mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mi>h</mml:mi><mml:mi>e</mml:mi><mml:mi>n</mml:mi></mml:mrow><mml:mo>-</mml:mo><mml:mrow><mml:msup><mml:mn>3.4</mml:mn><mml:mo>&#x00B0;</mml:mo></mml:msup><mml:mpadded width="+3.3pt"><mml:mtext>C</mml:mtext></mml:mpadded></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">&#x2264;</mml:mo><mml:mpadded width="+3.3pt"><mml:mi>T</mml:mi></mml:mpadded><mml:mo rspace="5.8pt">&lt;</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi>u</mml:mi><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:math></disp-formula>
<disp-formula id="S3.E6"><label>(6)</label><mml:math id="M6" display="block"><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi>r</mml:mi></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo rspace="5.8pt">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:mn>0</mml:mn></mml:mrow><mml:mo rspace="7.5pt">,</mml:mo><mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mi>h</mml:mi><mml:mi>e</mml:mi><mml:mpadded width="+5pt"><mml:mi>n</mml:mi></mml:mpadded><mml:mpadded width="+3.3pt"><mml:mi>T</mml:mi></mml:mpadded></mml:mrow><mml:mo rspace="5.8pt">&#x2265;</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi>u</mml:mi><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>where, R<sub>r</sub>(T) is the modeled rate of a rest break, T(t) is the air temperature, R<sub>r,obs</sub> is the rate of rest break observed in +6&#x00B0;C, and T<sub>upp</sub> is the upper threshold temperature.</p>
<p>For all the parameters in the overall model other than T<sub>upp</sub> and t<sub>0</sub> (start of the rest period), we obtained an estimate based on explicit experimental data from our study. Using those estimates in test simulations, we estimated the values of T<sub>upp</sub> and t<sub>0</sub> by minimizing the root mean square error (RMSE) between the predicted and the observed timing of bud burst in the nine treatments of the WTC experiment. For t<sub>0</sub>, we tested three values: November 1, November 15, and November 23. For T<sub>upp</sub>, we tested 15 values in the range of +4 to +20&#x00B0;C, with a step of 1&#x00B0;C.</p>
</sec>
<sec id="S2.SS4.SSS3">
<title>Sub-Model II</title>
<p>For any constant temperature T&#x2032;, the empirical value of the potential rate of ontogenetic development was calculated as (<xref ref-type="bibr" rid="B56">Sarvas, 1972</xref>; <xref ref-type="bibr" rid="B6">Campbell, 1978</xref>; <xref ref-type="bibr" rid="B69">Zhang et al., 2021c</xref>)</p>
<disp-formula id="S3.E7"><label>(7)</label><mml:math id="M7" display="block"><mml:mrow><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>o</mml:mi><mml:mo>,</mml:mo><mml:mrow><mml:mi>p</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mrow></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msup><mml:mi>T</mml:mi><mml:mo>&#x2032;</mml:mo></mml:msup><mml:mo rspace="5.8pt">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:mrow><mml:mn>100</mml:mn><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:mi>D</mml:mi><mml:mi>B</mml:mi><mml:mi>B</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:mrow></mml:mfrac></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>where, DBB = days to bud burst (leaf-out) required under the experimental temperature T&#x2032;.</p>
<p>As a result of using the multiplier 100, the scale for the ontogenetic development is the percentage scale [0,100%], so the value of R<sub>o,pot</sub> calculated with Equation (7) indicates the percentage of ontogenetic development, out of the total ontogenetic development required for leaf-out, taking place in a day. The value of DBB, initially expressed in terms of days, was converted to hours by multiplying the original value by 24, because the model was applied with a time step of 1 h.</p>
<p>The spring experiment produced the DBB data for Equation (7) should be started as close as possible to the time of rest completion under natural conditions (refer to section &#x201C;Constructing the sub-models on the basis of experimental data&#x201D; above). The time of rest completion under natural conditions was estimated in the autumn experiment using a chilling treatment under outdoor natural conditions. In that treatment, the DBB curve did not show leveling off even in the latest transfers from the chilling to the forcing conditions. Accordingly, following <xref ref-type="bibr" rid="B69">Zhang et al. (2021c)</xref>, we determined the &#x0394;t for the natural chilling treatment as follows: first, equation (2) was fitted to the scatter plot in a way similar to that used with the controlled chilling data. Using the fitted curve, the value of &#x0394;t was determined as the duration of chilling corresponding to the same value of DBB as was obtained with the +6&#x00B0;C treatment by the leveling off of the DBB curve (refer to <xref ref-type="fig" rid="F1">Figure 1D</xref> in the section &#x201C;Results&#x201D;). The starting date of the first transfer (February 13) was the closest to the estimated time of rest completion under natural conditions so the results of the first transfer were used for constructing sub-model II (refer to section &#x201C;Results&#x201D;).</p>
<p>Using Equation (7), the DBB values obtained for the individual seedlings in the first transfer of the spring experiment were first converted into the corresponding values of R<sub>o,pot</sub>. The R<sub>o,pot</sub> values, thus, obtained were then plotted against the experimental temperature, and the following sigmoidal equation was fitted to the scatter plot (<xref ref-type="bibr" rid="B26">H&#x00E4;nninen, 1990</xref>; <xref ref-type="bibr" rid="B69">Zhang et al., 2021c</xref>):</p>
<disp-formula id="S3.E8"><label>(8)</label><mml:math id="M8" display="block"><mml:mrow><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi>o</mml:mi><mml:mo>,</mml:mo><mml:mrow><mml:mi>p</mml:mi><mml:mi>o</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mrow></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo rspace="5.8pt">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:mfrac><mml:msub><mml:mi>a</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:mrow><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mfrac><mml:mn>1</mml:mn><mml:msub><mml:mi>b</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mfrac><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>T</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow></mml:msup></mml:mrow></mml:mfrac></mml:mrow></mml:math></disp-formula>
<p>where, T(t) is the air temperature, and a<sub>2</sub>, b<sub>2</sub>, and c<sub>2</sub> are parameters determining the upper asymptote, the slope, and the inflexion point of the sigmoidal curve, respectively.</p>
</sec>
<sec id="S2.SS4.SSS4">
<title>Sub-Model III</title>
<p>In a chilling-forcing experiment, the empirical value of ontogenetic competence, C<sub>o</sub>, for any given duration of chilling, x days, is obtained by definition as the ratio of DBB at rest completion to its value at x days of chilling: C<sub>o</sub>(x) = DBB(&#x0394;t)/DBB(x) (<xref ref-type="bibr" rid="B69">Zhang et al., 2021c</xref>). However, this mathematics assumes that all seedlings show bud burst, so BB% = 100%. As in several earlier studies, this was not the case in our study; so, in order to account for the seedlings not showing bud burst after short durations of chilling, we set the value of C<sub>o</sub> to zero with chilling durations that showed a BB% value below 50%. In all, then, the empirical value of C<sub>o</sub> for a given chilling duration x was calculated as follows (<xref ref-type="bibr" rid="B69">Zhang et al., 2021c</xref>):</p>
<disp-formula id="S3.E13"><mml:math id="M13" display="block"><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>o</mml:mi></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo rspace="5.8pt">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:mn>0</mml:mn></mml:mrow><mml:mo rspace="7.5pt">,</mml:mo><mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mi>h</mml:mi><mml:mi>e</mml:mi><mml:mpadded width="+5pt"><mml:mi>n</mml:mi></mml:mpadded><mml:mi>B</mml:mi><mml:mrow><mml:mi>B</mml:mi><mml:mo>%</mml:mo></mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo rspace="5.8pt" stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">&lt;</mml:mo><mml:mrow><mml:mn>50</mml:mn><mml:mo>%</mml:mo></mml:mrow></mml:mrow></mml:mrow></mml:math></disp-formula>
<disp-formula id="S3.E9"><label>(9)</label><mml:math id="M9" display="block"><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>o</mml:mi></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo rspace="5.8pt">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi mathvariant="normal">&#x0394;</mml:mi><mml:mi>t</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow></mml:mfrac></mml:mrow><mml:mo rspace="7.5pt">,</mml:mo><mml:mrow><mml:mrow><mml:mi>w</mml:mi><mml:mi>h</mml:mi><mml:mi>e</mml:mi><mml:mpadded width="+5pt"><mml:mi>n</mml:mi></mml:mpadded><mml:mi>B</mml:mi><mml:mrow><mml:mi>B</mml:mi><mml:mo>%</mml:mo></mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo rspace="5.8pt" stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">&#x2265;</mml:mo><mml:mrow><mml:mn>50</mml:mn><mml:mo>%</mml:mo></mml:mrow></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>where, f<sub>1</sub> is the function from equation (2).</p>
<p>In order to formulate sub-model III, the empirical values of C<sub>o</sub>(x) obtained by means of Equation (9) were plotted against the corresponding values of the state of rest break, S<sub>r</sub>. The latter were calculated by integrating the rate of rest break, calculated with Equation (6), up to the end of day x. Subsequently, a piece-wise linear model was fitted to the data (<xref ref-type="bibr" rid="B69">Zhang et al., 2021c</xref>):</p>
<disp-formula id="S3.E14"><mml:math id="M14" display="block"><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>o</mml:mi></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>S</mml:mi><mml:mi>r</mml:mi></mml:msub><mml:mo rspace="5.8pt">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:mn>0</mml:mn></mml:mrow><mml:mo rspace="7.5pt">,</mml:mo><mml:mrow><mml:mpadded width="+3.3pt"><mml:msub><mml:mi>S</mml:mi><mml:mi>r</mml:mi></mml:msub></mml:mpadded><mml:mo rspace="5.8pt">&lt;</mml:mo><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mrow><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:math></disp-formula>
<disp-formula id="S3.E10"><label>(10)</label><mml:math id="M10" display="block"><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>o</mml:mi></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>S</mml:mi><mml:mi>r</mml:mi></mml:msub><mml:mo rspace="5.8pt">)</mml:mo></mml:mrow></mml:mrow><mml:mo rspace="5.8pt">=</mml:mo><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:msub><mml:mi>S</mml:mi><mml:mi>r</mml:mi></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mo>-</mml:mo><mml:mrow><mml:mn>&#x2005;100</mml:mn><mml:msub><mml:mi>a</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:mrow></mml:mrow></mml:mrow><mml:mo rspace="7.5pt">,</mml:mo><mml:mrow><mml:mpadded width="+3.3pt"><mml:msub><mml:mi>S</mml:mi><mml:mi>r</mml:mi></mml:msub></mml:mpadded><mml:mo rspace="5.8pt">&#x2265;</mml:mo><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mrow><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:math></disp-formula>
</sec>
</sec>
<sec id="S2.SS5">
<title>Model Calculations</title>
<sec id="S2.SS5.SSS1">
<title>Procedures Applied in All Calculations</title>
<p>All calculations with the process-based tree phenology model developed were started on t<sub>0</sub> = November 15 (for estimating the value of t<sub>0</sub>, refer to section &#x201C;Results&#x201D;). The model was run on an hourly basis using hourly temperature data as input for calculating the hourly values of R<sub>r</sub>(t) (Equation 6) and R<sub>o,pot</sub>(t) (Equation 8). The rate of ontogenetic development, R<sub>o</sub>(t), was calculated by multiplying R<sub>o,pot</sub>(t) by the ontogenetic competence, C<sub>o</sub>(t) (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1</xref>). The integrations for S<sub>r</sub>(t) and S<sub>o</sub>(t) were carried out numerically by summing up the hourly values of R<sub>r</sub>(t) and R<sub>o</sub>(t). The value of S<sub>r</sub>(t) was kept at 100% for the annual cycle being simulated once that value, indicating rest completion, was attained. In calculations involving several years, a new annual cycle was started on the next t<sub>0</sub> = November 15 by setting S<sub>r</sub>(t) = 0% and S<sub>o</sub>(t) = 0% once leaf-out had been predicted (S<sub>o</sub>(t) = 100%).</p>
<p>All model calculations and statistical analyses were conducted with R studio (R version 4.0.0; <xref ref-type="bibr" rid="B54">R Core Team, 2020</xref>).</p>
</sec>
<sec id="S2.SS5.SSS2">
<title>Tests of the Model and Analyses of the Dormancy Dynamics Predicted by It</title>
<p>As stated above, the values of the parameters t<sub>0</sub> and T<sub>upp</sub> were estimated by fitting the overall model to the air temperature measurements and leaf-out observations in the WTC experiment. At the same time, the accuracy of the model was examined by evaluating the RMSE, but due to the estimation of the values of the two parameters, this examination did not provide an entirely independent test of the accuracy of the model (internal validation).</p>
<p>Using the natural-temperature data collected in the outdoor seedling collection on our campus, the dormancy dynamics predicted by the model was illustrated by calculating and plotting the values of the state of rest break, S<sub>r</sub>, and the state of ontogenetic development, S<sub>o</sub>, for November 15, 2017, to the predicted time of leaf-out in spring 2018. The predicted timing of rest completion was compared with the one observed in the experiment with natural chilling (for the latter, refer to <xref ref-type="fig" rid="F1">Figure 1D</xref> in the section &#x201C;Results&#x201D;). Correspondingly, the predicted timing of leaf-out was compared with the one observed in the outdoor seedling collection. Observations of the seedlings under the outdoor chilling conditions were not used in formulating the model so this prediction provided an independent yet single test of the overall model.</p>
</sec>
<sec id="S2.SS5.SSS3">
<title>Scenario Analyses</title>
<p>We applied the process-based model developed in this study to scenario analyses where the effects of climatic warming were projected on (1) the timing of the leaf-out of the pecan seedlings and (2) the subsequent risk of cold damage to them. The scenario simulations were carried out over the period 2022&#x2013;2099 for the three locations: our research site Hangzhou, Hefei (31&#x00B0;51&#x2033;N,117&#x00B0;10&#x2033;E), and Nanping (27&#x00B0;20&#x2033;N,118&#x00B0;7&#x2033;E). Hangzhou and Hefei are located in the main pecan cultivation area in subtropical southeastern China, whereas pecan cultivation is less common at the southern location Nanping (<xref ref-type="bibr" rid="B70">Zhang et al., 2015</xref>).</p>
<p>For each location, the projections were calculated using the daily minimum and maximum temperatures from the warming scenarios RCP4.5 and RCP8.5 (<xref ref-type="bibr" rid="B46">Meinshausen et al., 2011</xref>; <xref ref-type="bibr" rid="B60">Thrasher et al., 2012</xref>). For Hangzhou, Hefei, and Nanping, they represented warming by 1.4 (4.8&#x00B0;C), 1.7 (5&#x00B0;C), and 1.8&#x00B0;C (4.1&#x00B0;C), respectively (The values in parentheses are those for RCP8.5). The hourly temperature values needed in the simulations were generated from the daily minimum and maximum temperatures following <xref ref-type="bibr" rid="B72">Zohner et al. (2020)</xref>. For both RCP4.5 and RCP8.5, the projected leaf-out dates, expressed as DOY values, were plotted against the simulation year, and a linear regression line, indicating the rate of advancing or delay of leaf-out over 2022&#x2013;2199, was fitted to the scatter plot of each warming scenario. In the fitting of the linear regression lines, it was assumed that the two lines representing the two warming scenarios for a given location had the same value for the first simulation year 2022. The value was calculated as the average of the DOY values projected for the two respective scenarios for the location. The interception parameter was fixed to meet this criterion. Subsequently, the slope parameter was estimated by fitting the line to the observations.</p>
<p>In order to examine the risk of damage caused by low temperatures (false spring risk), the occurrence of cold damage events was determined by examining whether the air temperature dropped below a critical threshold, T<sub>dam</sub>, of the damaging temperature range during a time window of 10 days before the projected leaf-out to May 31. In the absence of explicit data for T<sub>dam</sub>, the threshold T<sub>dam</sub> = +5&#x00B0;C was determined on the basis of earlier indicative results (<xref ref-type="bibr" rid="B34">Kaur et al., 2020</xref>) and on the basis of recent experiences from a pecan orchard (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 3</xref>). The cold damage was quantified for each year by its incidence (number of damaging days) and severity (the lowest temperature occurring during the day or days). Finally, the cold damage year percentage (CDY%) for the whole simulation was determined as the percentage of the years with projected cold damage out of the 79 years simulated.</p>
<p>We had no explicit data for determining the value of the parameter T<sub>upp</sub>. That is why a sensitivity analysis was carried out by calculating the CDY% values for four additional values of T<sub>upp</sub>, in addition to the estimated value of T<sub>upp</sub> = +13&#x00B0;C (refer to <xref ref-type="fig" rid="F4">Figure 4</xref> in the section &#x201C;Results&#x201D;). The tested T<sub>upp</sub> values ranged from +11 to +15&#x00B0;C, with a step of 1&#x00B0;C.</p>
</sec>
</sec>
</sec>
<sec sec-type="results" id="S3">
<title>Results</title>
<sec id="S3.SS1">
<title>Experimental Results and the Resulting Process-Based Leaf-Out Model</title>
<p>With both natural and controlled chilling, the bud burst percentage, BB%, increased significantly from 10% at zero days of chilling to 100% in the fourth transfer after 42 days of chilling (<xref ref-type="fig" rid="F1">Figures 1A,B</xref> and <xref ref-type="table" rid="T1">Table 1</xref>). The days to bud burst, DBB, decreased significantly with prolonged chilling, both natural and controlled (<xref ref-type="table" rid="T1">Table 1</xref>). For the controlled chilling, the decrease was clearly exponential, showing leveling off with long durations of chilling (<xref ref-type="fig" rid="F1">Figure 1C</xref>), whereas for natural chilling, the decrease in DBB with prolonged chilling was only slightly exponential, with no clear leveling off (<xref ref-type="fig" rid="F1">Figure 1D</xref>). In the spring experiment, DBB decreased significantly with increased forcing temperature (<xref ref-type="fig" rid="F2">Figure 2</xref> and <xref ref-type="table" rid="T1">Table 1</xref>). Furthermore, DBB also decreased significantly from the first transfer on February 13 to the last one on March 13 (<xref ref-type="fig" rid="F2">Figure 2</xref> and <xref ref-type="table" rid="T1">Table 1</xref>).</p>
<table-wrap position="float" id="T1">
<label>TABLE 1</label>
<caption><p>Statistical analysis of factors affecting the days to bud burst, DBB, and the bud burst percentage, BB%, in the autumn and spring experiments (BB% in the autumn experiment only).</p></caption>
<table cellspacing="5" cellpadding="5" frame="hsides" rules="groups">
<thead>
<tr>
<td valign="top" align="left"><bold>Experiment</bold></td>
<td valign="top" align="left"><bold>Factor</bold></td>
<td valign="top" align="center" colspan="2"><bold><italic>DBB</italic></bold><hr/></td>
<td valign="top" align="center" colspan="1"><bold><italic>BB%</italic></bold><hr/></td>
</tr>
<tr>
<td valign="top" align="justify"/>
<td/>
<td valign="top" align="center"><bold><italic>F</italic></bold></td>
<td valign="top" align="center"><bold><italic>P</italic></bold></td>
<td valign="top" align="center"><bold><italic>P</italic></bold></td>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Autumn experiment</td>
<td valign="top" align="left">Chilling type</td>
<td valign="top" align="center"><bold>27.7459</bold></td>
<td valign="top" align="center"><bold>&#x003C; 0.001</bold></td>
<td valign="top" align="center">0.993</td>
</tr>
<tr>
<td valign="top" align="justify"/>
<td valign="top" align="left">Transfer</td>
<td valign="top" align="center"><bold>38.9620</bold></td>
<td valign="top" align="center"><bold>&#x003C; 0.001</bold></td>
<td valign="top" align="center"><bold>&#x003C; 0.001</bold></td>
</tr>
<tr>
<td valign="top" align="justify"/>
<td valign="top" align="left">Transfer&#x002A;Chilling type</td>
<td valign="top" align="center">1.6253</td>
<td valign="top" align="center">0.642</td>
<td valign="top" align="center">0.955</td>
</tr>
<tr>
<td valign="top" align="justify"/>
<td valign="top" align="left">Transfer</td>
<td valign="top" align="center"><bold>23.446</bold></td>
<td valign="top" align="center"><bold>&#x003C; 0.001</bold></td>
<td/>
</tr>
<tr>
<td valign="top" align="left">Spring experiment</td>
<td valign="top" align="left">Temperature</td>
<td valign="top" align="center"><bold>189.461</bold></td>
<td valign="top" align="center"><bold>&#x003C; 0.001</bold></td>
<td/>
</tr>
<tr>
<td valign="top" align="justify"/>
<td valign="top" align="left">Transfer&#x002A;Temperature</td>
<td valign="top" align="center"><bold>3.014</bold></td>
<td valign="top" align="center"><bold>0.023</bold></td>
<td/>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn id="tfn1"><p><italic>A two-way ANOVA was applied to the analysis of the DBB results and logistic regression with a binary response of factors to the analysis of the BB% results. In the autumn experiment, the chilling type refers to the difference between chilling under controlled conditions at +6&#x00B0;C and chilling under natural outdoor conditions. The <italic>F</italic> and <italic>P</italic> values in bold indicate statistical significances with at least <italic>P</italic> &#x003C; 0.05.</italic></p></fn>
</table-wrap-foot>
</table-wrap>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption><p>Effects of air temperature on days to bud burst, DBB (mean &#x00B1; SE), of first-year pecan seedlings in the spring experiment. The transfer dates indicate the time when the seedlings were transferred from the outdoor natural overwintering conditions to the three growth chambers with respective forcing temperatures of +10, +17, and +24&#x00B0;C. Note that the phenological event observed was leaf-out, but that the concept &#x201C;bud burst&#x201D; is used here as a generic one facilitating the use of the standard index DBB.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-12-768963-g002.tif"/>
</fig>
<p>For constructing sub-model I, the value of &#x0394;t = 64 days was obtained in the autumn experiment for the duration of chilling required for rest break in the controlled chilling at constant +6&#x00B0;C (<xref ref-type="fig" rid="F1">Figure 1C</xref>). On an hourly basis, this implies an empirical rate of rest break R<sub>r,obs</sub> = 100%/(64 days &#x00D7; 24 h day<sup>&#x2013;1</sup>) = .065% h<sup>&#x2013;1</sup> at +6&#x00B0;C (Equation 1; <xref ref-type="fig" rid="F3">Figure 3A</xref> and <xref ref-type="table" rid="T2">Table 2</xref>).</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption><p>The three sub-models constitute the process-based leaf-out phenology model developed in this study for first-year pecan seedlings. <bold>(A)</bold> Sub-model I: air temperature response of the rate of a rest break, R<sub>r</sub>, (Equation 6). <bold>(B)</bold> Sub-model II: air temperature response of the potential rate of ontogenetic development, R<sub>o,pot</sub>, (Equation 8). <bold>(C)</bold> Sub-model III: dependence of ontogenetic competence, C<sub>o</sub>, on the state of rest break, S<sub>r</sub>, (Equation 10). For the structure of the overall model and the relationships between the sub-models, refer to <xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1</xref>. The red dots represent the empirical data points calculated based on results from the autumn and spring experiments (<xref ref-type="fig" rid="F1">Figures 1</xref>, <xref ref-type="fig" rid="F2">2</xref>) and the black lines and curves the response functions fitted to the data points. For the equations and details of constructing the models, refer to &#x201C;Constructing the sub-models on the basis of experimental data&#x201D; in the section &#x201C;Materials and Methods.&#x201D; The parameter values of the models can be found in <xref ref-type="table" rid="T2">Table 2</xref>.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-12-768963-g003.tif"/>
</fig>
<table-wrap position="float" id="T2">
<label>TABLE 2</label>
<caption><p>Parameter values of the process-based leaf-out phenology model developed in this study for first-year seedlings of subtropical pecan.</p></caption>
<table cellspacing="5" cellpadding="5" frame="hsides" rules="groups">
<thead>
<tr>
<td valign="top" align="left"><bold>Sub model</bold></td>
<td valign="top" align="center"><bold>Parameter</bold></td>
<td valign="top" align="center"><bold>Value</bold></td>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Overall model</td>
<td valign="top" align="center">t<sub>0</sub></td>
<td valign="top" align="center">15 November</td>
</tr>
<tr>
<td valign="top" align="left">Sub-model I</td>
<td valign="top" align="center">T<sub>upp</sub></td>
<td valign="top" align="center">+13&#x00B0;C</td>
</tr>
<tr>
<td/>
<td valign="top" align="center">R<sub>r,obs</sub></td>
<td valign="top" align="center">0.065% per hour</td>
</tr>
<tr>
<td valign="top" align="left">Sub-model II</td>
<td valign="top" align="center">a<sub>2</sub></td>
<td valign="top" align="center">0.287</td>
</tr>
<tr>
<td/>
<td valign="top" align="center">b<sub>2</sub></td>
<td valign="top" align="center">&#x2212;5.999</td>
</tr>
<tr>
<td/>
<td valign="top" align="center">c<sub>2</sub></td>
<td valign="top" align="center">21.64</td>
</tr>
<tr>
<td valign="top" align="left">Sub-model III</td>
<td valign="top" align="center">a<sub>3</sub></td>
<td valign="top" align="center">0.0079279</td>
</tr>
<tr>
<td/>
<td valign="top" align="center">S<sub>r,min</sub></td>
<td valign="top" align="center">14%</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn id="tfn2"><p><italic>Sub-model I: air temperature response of the rate of rest break, R<sub><italic>r</italic></sub> (Equation 6, <xref ref-type="fig" rid="F3">Figure 3A</xref>). Sub-model II: air temperature response of the potential rate of ontogenetic development, R<sub><italic>o,pot</italic></sub>(Equation 8, <xref ref-type="fig" rid="F3">Figure 3B</xref>). Sub-model III: dependence of ontogenetic competence, C<sub><italic>o</italic></sub>, on the state of rest break, S<sub><italic>r</italic></sub> (Equation 10, <xref ref-type="fig" rid="F3">Figure 3C</xref>). For the structure of the overall model, refer to <xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 1</xref>.</italic></p></fn>
</table-wrap-foot>
</table-wrap>
<p>The upper threshold, T<sub>upp</sub>, of the rest-breaking temperature range in sub-model I was estimated by fitting the overall model (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figures 1</xref>, <xref ref-type="supplementary-material" rid="DS1">3</xref>) to the leaf-out observations in the WTC experiment (<xref ref-type="fig" rid="F4">Figure 4</xref>). Simultaneously, the value of parameter t<sub>0</sub>, starting day of rest period, was estimated by carrying out the calculations for estimating T<sub>upp</sub> with three different values of t<sub>0</sub>. The values of RMSE obtained for the three t<sub>0</sub> values November 1, November 15, and November 23 were 2.11, 1.67, and 2.24 days, respectively, implying the value of 15 November for t<sub>0</sub> (<xref ref-type="table" rid="T2">Table 2</xref>). Using that value of t<sub>0</sub>, the RMSE between the predicted and the observed timing of leaf-out was minimized with T<sub>upp</sub> = +13&#x00B0;C (<xref ref-type="fig" rid="F4">Figure 4</xref>); so, that value was adopted as the estimate of T<sub>upp</sub> (<xref ref-type="table" rid="T2">Table 2</xref>).</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption><p>Estimation of the upper threshold of the rest-breaking temperature range, T<sub>upp</sub> (refer to <xref ref-type="fig" rid="F3">Figure 3A</xref>) by fitting the overall model to the results of the nine temperature treatments of the whole-tree chamber (WTC) experiment. The graph shows the root mean square error (RMSE) of the leaf-out timing predicted by the overall model for the experiment as a function of the value of T<sub>upp</sub> used in the simulations. With each value of T<sub>upp</sub>, the calculations were started on t<sub>0</sub> = November 15, because the use of that date minimized the RMSE among the dates tested (refer to the section &#x201C;Results&#x201D; in the text). With the lowest value of T<sub>upp</sub> tested (+6&#x00B0;C), the model failed to predict any leaf-out for three of the nine temperature treatments in the experiment because of insufficient chilling. This is why no RMSE is given for T<sub>upp</sub> = +6&#x00B0;C.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-12-768963-g004.tif"/>
</fig>
<p>Sub-model II addresses the air temperature response of the potential rate of ontogenetic development, R<sub>o,pot</sub>. This implies that the experiment for determining sub-model II should be started as close as possible to the estimated time of rest completion under natural conditions (refer to &#x201C;Constructing the sub-models on the basis of experimental data&#x201D; in the section &#x201C;Materials and Methods&#x201D;). In the autumn experiment, rest completion under natural conditions was estimated to take place at &#x0394;t = 90 days after the onset of the experiment on November 21, 2017 (<xref ref-type="fig" rid="F1">Figure 1D</xref>), i.e., February 19, 2018. This means that the first (February 13), second (February 27), and third transfers (March 13) in the spring experiment (<xref ref-type="fig" rid="F2">Figure 2</xref>) were carried out 6 days before, 8 days after, and 22 days after the estimated rest completion, respectively. Accordingly, the results of the first transfer in the spring experiment (<xref ref-type="fig" rid="F2">Figure 2</xref>) were used in the construction of sub-model II (<xref ref-type="fig" rid="F3">Figure 3B</xref> and <xref ref-type="table" rid="T2">Table 2</xref>).</p>
<p>The empirical value of ontogenetic competence, C<sub>o</sub>, was zero in the first transfer with S<sub>r</sub> = 0% (<xref ref-type="fig" rid="F3">Figure 3C</xref>). This was because of the low value of BB% in the first transfer (<xref ref-type="fig" rid="F1">Figure 1A</xref>; refer to Equation 9). Starting from the second transfer, the empirical value of C<sub>o</sub> increased with increasing S<sub>r</sub> (= with prolonged chilling). Accordingly, a piece-wise linear relationship with a discontinuity at S<sub>r,min</sub> = 14% was determined for sub-model III (<xref ref-type="fig" rid="F3">Figure 3C</xref> and <xref ref-type="table" rid="T2">Table 2</xref>).</p>
</sec>
<sec id="S3.SS2">
<title>Model Test and Predictions</title>
<p>According to the model prediction for the dormancy dynamics for the period of autumn 2017 to spring 2018, rest break started immediately at the beginning of the simulation in November 2017, as shown by the increasing value of the state of rest break, S<sub>r</sub>, at that time (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 4B</xref>). This was because the air temperature (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 4A</xref>) at the time fluctuated mainly in the range causing rest break (<xref ref-type="fig" rid="F3">Figure 3A</xref>). The simulated rest break progressed at an almost constant rate, leading to predicted rest completion on February 1, 2019, 20 days before the independently observed rest completion on February 21 (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 4B</xref>), estimated on the basis of the autumn experiment results (<xref ref-type="fig" rid="F1">Figure 1D</xref>). No ontogenetic development was predicted for the beginning of the simulation, as shown by the values of S<sub>o</sub> = 0% at that time (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 4B</xref>). That was because with S<sub>r</sub> &#x003C; 14%, the ontogenetic competence stayed at C<sub>o</sub> = 0 (<xref ref-type="fig" rid="F3">Figure 3C</xref>; ontogenetic competence not shown in <xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 4B</xref>). With further rest break beyond S<sub>r</sub> = 14%, ontogenetic development also started, but the S<sub>o</sub> increased slowly at first because the ontogenetic competence was still relatively low and the air temperatures (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 4A</xref>) were generally too low to promote ontogenetic development (refer to <xref ref-type="fig" rid="F3">Figure 3B</xref>). Toward spring, the predicted rate of ontogenetic development increased, and leaf-out was predicted to occur on April 2, 2018, 1 day after leaf-out was independently observed under natural conditions (<xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 4B</xref>).</p>
<p>The results presented in <xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 4</xref> provide an independent test of our model with observational data. However, as only 1 year was included in the test, the test is relatively weak, but it serves to illustrate the dormancy dynamics predicted by our process-based leaf-out model. In the main test, the model simulated the timing of leaf-out in the nine treatments of the WTC experiment with good accuracy (RMSE = 1.67 days, <xref ref-type="fig" rid="F5">Figure 5</xref>).</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption><p>Test of the process-based leaf-out phenology model developed in this study for first-year pecan seedlings by leaf-out observations from a WTC experiment with nine temperature treatments.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-12-768963-g005.tif"/>
</fig>
</sec>
<sec id="S3.SS3">
<title>Projections of Leaf-Out Timing and Cold Damage for Climatic Warming</title>
<p>For both RCP4.5 and RCP8.5, our model projected an overall advancing trend in pecan seedling leaf-out in all three locations addressed (<xref ref-type="fig" rid="F6">Figure 6</xref>). There were, however, considerable differences between the locations and the warming scenarios. For the two northern locations Hangzhou and Hefei, an overall advancement at rates of about &#x2212;1 and &#x2212;1.5 days per decade, respectively, was projected under RCP4.5 (<xref ref-type="fig" rid="F6">Figures 6A,C</xref>), and the rate was about double under RCP8.5 (<xref ref-type="fig" rid="F6">Figures 6B,D</xref>). In the southern location Nanping, the advancement rate was about &#x2212;1.5 days per decade under RCP4.5 and slightly smaller (less negative) under RCP8.5 (<xref ref-type="fig" rid="F6">Figures 6E,F</xref>). In all three locations, there was more year-to-year variation in the timing of leaf-out under RCP8.5 than under RCP4.5 (<xref ref-type="fig" rid="F6">Figure 6</xref>). In the southern location Nanping, the large year-to-year variation led to a delay in leaf-out in many years during the first decades of the 21st century despite the overall advancement trend (<xref ref-type="fig" rid="F6">Figure 6F</xref>).</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption><p>Projected timing of leaf-out in first-year pecan seedlings in three locations in subtropical southeastern China from 2021 to 2099. Using the process-based phenology model developed in this study, the leaf-out was projected for the warming scenarios RCP4.5 (panels on the left) and RCP8.5 (panels on the right) for <bold>(A,B)</bold> Hangzhou and <bold>(C,D)</bold> Hefei, located in the main pecan cultivation area in the northern part of the subtropical monsoon climate zone, and for <bold>(E,F)</bold> Nanping, located south of the main pecan cultivation area. &#x201C;&#x002A;&#x002A;&#x002A;&#x201D; indicates significance at <italic>P</italic> &#x003C; 0.001.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-12-768963-g006.tif"/>
</fig>
<p>Our model projected no cold damage for Hangzhou under RCP4.5 (cold damage year percentage CDY% = 0), and under RCP8.5, projected cold damage was rare (CDY% = 3.8) (<xref ref-type="fig" rid="F7">Figure 7A</xref>). Projected cold damage was also quite rare in Hefei, with the CDY% values at 5.1 and 6.4 for RCP4.5 and RCP8.5, respectively (<xref ref-type="fig" rid="F7">Figure 7B</xref>). For Nanping, much more frequent cold damage was projected, and contrary to the two northern locations, there was more projected cold damage under RCP4.5 (CDY% = 16.7) than under RCP8.5 (CDY% = 9) (<xref ref-type="fig" rid="F7">Figure 7C</xref>). No clear differences among the three locations were found in the annual indices of cold damage (incidence and severity), with the following two exceptions: first, in the simulation for Nanping under RCP4.5, there was one exceptional year with an exceptionally high incidence (4 days) of cold damage (<xref ref-type="fig" rid="F7">Figure 7C</xref>). This is in line with the projection of cold damage being common in Nanping (CDY% = 16.7) under RCP4.5. Second, even though cold damage was projected for only 3 years in Hangzhou under RCP8.5 (CDY% = 3.8), it was more severe in Hangzhou than in the other two locations in one of those years (<xref ref-type="fig" rid="F7">Figure 7</xref>).</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption><p>Projected cold damage to the first-year pecan seedlings in three locations in subtropical southeastern China from 2021 to 2099 under the warming scenarios RCP4.5 (red symbols) and RCP8.5 (blue symbols).<bold>(A)</bold> Hangzhou and <bold>(B)</bold> Hefei are located in the main pecan cultivation area in the northern part of the subtropical monsoon climate zone and <bold>(C)</bold> Nanping south of the main pecan cultivation area. The cold damage was projected by examining whether the air temperature dropped below the threshold of +5&#x00B0;C during the time window from 10 days before the projected leaf-out (<xref ref-type="fig" rid="F6">Figure 6</xref>) to May 31. If cold damage was projected for a given year, it was quantified by its incidence (number of days when damaging air temperatures occurred: triangles, vertical axis on the left-hand side), and severity (the lowest temperature that occurred during those days: squares, vertical axis on the right-hand side). In order to make both cold damage indices increase from the bottom to the top of the panels, the severity is expressed by the opposite number of the corresponding temperature. The values of CDY% in red and blue indicate the percentage of cold damage years for the respective warming scenarios out of the 79 years simulated.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-12-768963-g007.tif"/>
</fig>
<p>In the sensitivity analysis, only a minor effect of the parameter T<sub>upp</sub> on the CDY% values was found for Hangzhou and Hefei, indicating that our results for these two locations are robust (<xref ref-type="supplementary-material" rid="DS1">Supplementary Table 1</xref>). For Nanping, however, low values of T<sub>upp</sub> (+11 and +12&#x00B0;C) decreased the CDY%, and high values of T<sub>upp</sub> (+14 and +15&#x00B0;C) increased it in comparison with the CDY% values obtained in the main simulation with the estimated value of T<sub>upp</sub> = +13&#x00B0;C (<xref ref-type="supplementary-material" rid="DS1">Supplementary Table 1</xref>).</p>
</sec>
</sec>
<sec sec-type="discussion" id="S4">
<title>Discussion</title>
<sec id="S4.SS1">
<title>Biological Realism of the Process-Based Tree Phenology Models</title>
<p><xref ref-type="bibr" rid="B59">Sparks (1993)</xref> demonstrated experimentally the existence of rest period (endodormancy) and chilling requirement for pecan trees growing over a large geographical range in the United States. Our experimental findings confirm that seedlings of the subtropical pecan grown in southeastern China also evince these traits. This is in line with recent studies, which show that several subtropical tree species have a rest period and a chilling requirement (<xref ref-type="bibr" rid="B19">Du et al., 2019</xref>; <xref ref-type="bibr" rid="B58">Song et al., 2020</xref>; <xref ref-type="bibr" rid="B50">Pan et al., 2021</xref>; <xref ref-type="bibr" rid="B67">Zhang et al., 2021a</xref>, <xref ref-type="bibr" rid="B68">b</xref>). The novelty and scarcity of these findings in the case of subtropical trees are in striking contrast with the case of boreal and temperate trees, where the existence of these traits has already been known for a 100 years (<xref ref-type="bibr" rid="B18">Coville, 1920</xref>; <xref ref-type="bibr" rid="B33">Jewaria et al., 2021</xref>).</p>
<p>We introduced a process-based spring leaf-out model for the subtropical first-year pecan seedlings we examined in this study. Our main emphasis was on the biological realism of the models (<xref ref-type="bibr" rid="B39">Levins, 1966</xref>, <xref ref-type="bibr" rid="B40">1968</xref>; <xref ref-type="bibr" rid="B12">Charrier et al., 2015</xref>; <xref ref-type="bibr" rid="B29">H&#x00E4;nninen, 2016</xref>), which is why the model development was based on a hypothetico-deductive (HDM) approach, which makes use of experiments explicitly designed for examining the responses modeled (sub-models I&#x2013;III). The approach is regarded as an HDM one because the model development is based on the implications of the models for the occurrence and timing of the readily observable leaf-out under experimental conditions rather than direct observations and measurements of the modelled physiological and morphological phenomena of rest break and ontogenetic development. Accordingly, all the data points in <xref ref-type="fig" rid="F3">Figure 3</xref> are determined by analyzing the leaf-out data gathered under the experimental conditions.</p>
<p>This approach, referred to as the ecophysiological approach by <xref ref-type="bibr" rid="B29">H&#x00E4;nninen (2016)</xref>, has been taken in process-based tree phenology modeling only rarely (<xref ref-type="bibr" rid="B56">Sarvas, 1972</xref>, <xref ref-type="bibr" rid="B57">1974</xref>; <xref ref-type="bibr" rid="B7">Campbell and Sugano, 1975</xref>, <xref ref-type="bibr" rid="B8">1979</xref>; <xref ref-type="bibr" rid="B5">Caffarra et al., 2011</xref>; <xref ref-type="bibr" rid="B69">Zhang et al., 2021c</xref>). This is obviously because the experiments are time-consuming and laborious. Most earlier studies with process-based tree phenology modeling have been based on the technique of inverse modeling, where the model parameters are estimated by fitting the model to observational long-term phenological and air temperature records (<xref ref-type="bibr" rid="B36">Kramer, 1994</xref>; <xref ref-type="bibr" rid="B15">Chuine et al., 1998</xref>; <xref ref-type="bibr" rid="B1">Basler, 2016</xref>; this is a phenological approach in the terminology of <xref ref-type="bibr" rid="B29">H&#x00E4;nninen, 2016</xref>).</p>
<p>This is unfortunate, for it has been known since the pioneering study of <xref ref-type="bibr" rid="B32">Hunter and Lechowicz (1992)</xref> that inverse modeling with observational data runs a high risk of producing biologically unrealistic process-based models of tree phenology. To take just two different examples of the problems related to inverse modeling (for a review of the problems, refer to <xref ref-type="bibr" rid="B31">H&#x00E4;nninen et al., 2019</xref>), first, by applying inverse modeling to the growth onset of Scots pine (<italic>Pinus sylvestris</italic>) saplings in a warming experiment, <xref ref-type="bibr" rid="B28">H&#x00E4;nninen (1995)</xref> found that a model based on photoperiod outcompeted all models in which chilling causes rest break. However, in an explicit experiment where photoperiod was controlled, he found that photoperiod does not affect the rest break of Scots pine saplings at all. The cause of the problem was that in the warming experiment the natural photoperiod correlated with chilling accumulation, which actually caused the rest break. Second, using an inverse modeling approach, <xref ref-type="bibr" rid="B42">Luedeling et al. (2021)</xref> recently found that temperatures of up to +30&#x00B0;C cause rest breaks in apples (<italic>Malus domestica</italic>). As discussed by the authors themselves, this result is most probably an artifact caused by the lack of temperatures above +10&#x00B0;C in the observational data set.</p>
<p>Despite the experimental approach taken, our model still needs further testing and development. This is especially true in the case of sub-model I, where we had just one empirical data point for the model. This is where our study deviated most from the study of <xref ref-type="bibr" rid="B69">Zhang et al. (2021c)</xref>, which we otherwise followed closely in building the model on the basis of experimental data. We solved the problem following <xref ref-type="bibr" rid="B43">Lundell et al. (2020)</xref>, who also had just one controlled chilling temperature in their experiment: (1) the lower threshold of the rest-breaking temperature range was set at &#x2212;3.4&#x00B0;C (<xref ref-type="bibr" rid="B57">Sarvas, 1974</xref>), (2) the upper threshold T<sub>upp</sub> was estimated using an inverse modeling approach of fitting the model to the experimental results, and (3) a plateau response was assumed between the two threshold temperatures. In this way, we obtained a reasonable fit of the overall model to the experimental results (<xref ref-type="fig" rid="F5">Figure 5</xref>). It should also be noted that in the mainline inverse modeling approach that uses observational phenological records (<xref ref-type="bibr" rid="B36">Kramer, 1994</xref>; <xref ref-type="bibr" rid="B15">Chuine et al., 1998</xref>; <xref ref-type="bibr" rid="B1">Basler, 2016</xref>), there are no experimentally determined data points available for estimating the value of any parameter of any sub-model.</p>
<p>Our estimated value of T<sub>upp</sub> = +13&#x00B0;C is higher than the upper thresholds usually applied in process-based models for boreal and temperate trees (<xref ref-type="bibr" rid="B57">Sarvas, 1974</xref>; <xref ref-type="bibr" rid="B10">Cannell and Smith, 1983</xref>; <xref ref-type="bibr" rid="B64">Wang et al., 2020</xref>; <xref ref-type="bibr" rid="B66">Xu et al., 2020</xref>). However, the value is well in line with the experimental results available for subtropical trees. <xref ref-type="bibr" rid="B67">Zhang et al. (2021a</xref>, <xref ref-type="bibr" rid="B69">c)</xref> found that in two subtropical tree species the rest-breaking effect of +15&#x00B0;C was equal to that of +10 and +5&#x00B0;C, suggesting that in subtropical trees T<sub>upp</sub> can even be well above +15&#x00B0;C (refer to also <xref ref-type="bibr" rid="B33">Jewaria et al., 2021</xref>). Further experimental studies with several controlled chilling temperatures and chilling durations (<xref ref-type="bibr" rid="B3">Baumgarten et al., 2021</xref>; <xref ref-type="bibr" rid="B67">Zhang et al., 2021a</xref>, <xref ref-type="bibr" rid="B69">c</xref>) are needed to test and improve the sub-model I developed for pecan seedlings in this study.</p>
<p>The starting date of the rest period (endodormancy) used in this study (t<sub>0</sub> = November 15) also involves a great deal of uncertainty. In that respect, our model is no exception among the published process-based tree phenology models. To the best of our knowledge, the value of t<sub>0</sub> is not based on explicit ecophysiological data in any of them (but refer to <xref ref-type="bibr" rid="B24">Fuchigami et al., 1982</xref> and the related discussion in <xref ref-type="bibr" rid="B29">H&#x00E4;nninen, 2016</xref>, p. 119&#x2013;120). Arbitrary starting dates, such as September 1 (<xref ref-type="bibr" rid="B26">H&#x00E4;nninen, 1990</xref>, <xref ref-type="bibr" rid="B27">1991</xref>; <xref ref-type="bibr" rid="B15">Chuine et al., 1998</xref>, <xref ref-type="bibr" rid="B14">2016</xref>) and November 1 (<xref ref-type="bibr" rid="B10">Cannell and Smith, 1983</xref>; <xref ref-type="bibr" rid="B36">Kramer, 1994</xref>), have been used with boreal and temperate trees earlier on. In subtropical trees, bud set typically occurs from September to October (<xref ref-type="bibr" rid="B67">Zhang et al., 2021a</xref>), which is why we used November 1 as the first candidate when estimating the value of t<sub>0</sub>.</p>
<p>For our experiments, we used seedlings raised from seeds collected in the seminatural pecan forests of our study area in the Hangzhou region. It is well-known that seminatural pecan trees are of subtropical origin, but no exact information about their genetic background is available (<xref ref-type="bibr" rid="B70">Zhang et al., 2015</xref>). In pecan nut prediction, bred cultivars are normally used, which implies that the generality of our model should also be tested with bred cultivars in future studies.</p>
</sec>
<sec id="S4.SS2">
<title>Projected Effects of Climatic Warming</title>
<p>Depending on the geographical location, the warming scenario, and the year of simulation, all three of our hypotheses gained support from some part of our simulation results. This even held for the delay hypothesis, for in many years of the first decades of the 21st century, leaf-out was delayed in the simulations for the southern location Nanping under the RCP8.5 warming scenario, despite the overall advancement trend found for Nanping under RCP8.5. For most years, however, advancement of leaf-out was projected for all the three locations and under both climatic scenarios addressed. In comparison with earlier studies with temperate trees (<xref ref-type="bibr" rid="B36">Kramer, 1994</xref>; <xref ref-type="bibr" rid="B49">Murray et al., 1994</xref>; <xref ref-type="bibr" rid="B64">Wang et al., 2020</xref>), the advancement rates found in this study were relatively low. This suggests that reduced chilling restricts the advancement of spring phenology more under the warm subtropical conditions than under the cooler temperate conditions.</p>
<p>A clear although not very rapid advancement of leaf-out was projected for the two northern locations, Hangzhou and Hefei. This held for both RCP4.5 and RCP8.5, and the rate of advancement under RCP8.5 was about double the rate under RCP4.5. These results show that in Hangzhou and Hefei, the effect of increased forcing overrode the effect of decreased chilling on the projected timing of leaf-out. For these two locations, cold damage was projected quite infrequently: once every 26 years (CDY% = 3.8%) at most in Hangzhou and once every 16 years (CDY% = 6.4%) in Hefei. In all, despite some cold damage projected, the prolonged growing season hypothesis was mainly supported by our findings for Hangzhou and Hefei.</p>
<p>The results projected for the southern location Nanping deviated from those found for the two northern locations in many ways. First, the advancement rate of leaf-out in Nanping was almost identical for the two warming scenarios. This showed that the effect of reduced chilling was stronger effect under the warming of the warmer climate in Nanping than under the warming of the cooler climates of the two northern locations and that Nanping is ultimately receiving less chilling with warming, which is impacting leaf-out timing. Second, as the projected advancement rates for Nanping were quite similar under the two climatic scenarios, more cold damage was projected under RCP4.5 than under the warmer scenario of RCP8.5. In Nanping, the value of CDY% was 16.7 for RCP4.5 and 9 for RCP8.5, implying that cold damage would occur once every 6 (RCP4.5) or once every 11 (RCP8.5) years. However, the results of the sensitivity analysis show a higher uncertainty for Nanping than for the other two locations. For Nanping, much less cold damage was projected for the low values (+11 and +12&#x00B0;C) of T<sub>upp</sub> than for the estimated value of it (T<sub>upp</sub> = +13&#x00B0;C) (<xref ref-type="supplementary-material" rid="DS1">Supplementary Table 1</xref>). This finding emphasizes the need for further experimental studies to improve sub-model I (refer to above).</p>
<p>In Nanping, CDY% was exceptionally higher under the cooler scenario RCP4.5 than under the warmer scenario RCP8.5. This was caused by the similar timing of leaf-out projected in Nanping for the two climatic scenarios. In other words, if leaf-out occurs simultaneously in a cooler and a warmer climate, then probably there is more cold damage in the cooler than in the warmer climate. For Nanping, then, a paradoxical conclusion arises: warming as such causes cold damage by false springs, but rapid warming causes such damage less than slow warming because with rapid warming the climate gets so warm after some decades that the potentially damaging temperatures below +5&#x00B0;C do not occur around the time of leaf-out any longer. This is why the projected damage in Nanping under RCP8.5 concentrates on the early decades, whereas under RCP4.5 cold damage is also projected for the late years. A similar phenomenon was actually found for Hefei; however, the results for Hefei were different in other respects (refer to the previous paragraph). This finding suggests that in the southern part of the subtropical zone, where the climate is relatively warm already, rapid warming creates a time window of high risks of false springs for a few decades. After the time window closes, the risk of cold damage decreases.</p>
<p>The modeling approach adopted in this study has been applied earlier for assessing the effects of climatic warming on spring phenology and the risk of false springs in various boreal and temperate trees (<xref ref-type="bibr" rid="B9">Cannell, 1985</xref>; <xref ref-type="bibr" rid="B27">H&#x00E4;nninen, 1991</xref>; <xref ref-type="bibr" rid="B36">Kramer, 1994</xref>; <xref ref-type="bibr" rid="B41">Linkosalo et al., 2000</xref>). The approach holds great potential for assessing the suitability of perennial horticultural crops for cultivation under climatic warming at different geographical locations. For instance, under climatic warming, many subtropical crops may find new cultivation areas under temperate conditions. The present modeling approach is well-suited for assessing the suitability of subtropical crops to such transfers to temperate conditions.</p>
</sec>
</sec>
<sec sec-type="conclusion" id="S5">
<title>Conclusion</title>
<p>We introduced a process-based phenology model for the leaf-out of pecan seedlings grown in subtropical southeastern China. In order to maximize the biological realism of the model, we based its development on experiments explicitly addressing the responses of the developmental phenomena modeled. The model was applied to project the timing of leaf-out and risk of false spring in two locations in the current main pecan cultivation area in the northern part of the subtropical monsoon climate zone in southeastern China and one location south of the main cultivation area. An overall advancement of leaf-out was projected for all three locations. For the two northern locations in the main cultivation area, no considerable increase in cold damage caused by false springs was projected. This finding suggests that pecan cultivation can continue relatively safely in these locations in the upcoming decades, too, even though under the RCP8.5 warming scenario, damage caused by false spring was projected to occur once every 16&#x2013;26 years in these two northern locations, too. Paradoxically, cold damage caused by false springs was projected to occur more frequently in the southern location, once every 6 and 11 years under the warming scenarios RCP4.5 and RCP8.5, respectively. Due to the uncertainties related to the air temperature response of rest break (endodormancy release) to chilling, our conclusions need to be further addressed in further experimental studies and model development based on it. Similarly, the uncertainties related to the genetic background of our research material should be addressed by testing our model with pecan cultivars used in commercial nut production. On the basis of our present results, we do not recommend starting large-scale pecan cultivation in locations south of the present main pecan cultivation area in southeastern subtropical China.</p>
</sec>
<sec sec-type="data-availability" id="S6">
<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">
<title>Author Contributions</title>
<p>RZ designed the study. JZ, JL, and SS carried out the experiments. JZ, RZ, and HH analyzed the data and carried out the modeling. JZ, HH, and RZ wrote the manuscript. All authors contributed to the article and approved the submitted version.</p>
</sec>
<sec sec-type="COI-statement" id="conf1">
<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 sec-type="disclaimer" id="pudiscl1">
<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>
</body>
<back>
<sec sec-type="funding-information" id="S8">
<title>Funding</title>
<p>This study was financed by the National Natural Science Foundation of China (32171832 and 31800579), the Youth Elite Science Sponsorship Program of CAST (YESS, 2020QNRC001), the National Forestry and Grassland Technological Innovation Program for Young TopNotch Talents (2020132604), the Key Research Program of Zhejiang Province (2018C02004), and Overseas Expertise Introduction Project for Discipline Innovation (111 Project D18008).</p>
</sec>
<ack>
<p>We thank Xianlin Feng for providing the photograph and temperature data shown in <xref ref-type="supplementary-material" rid="DS1">Supplementary Figure 3</xref>. We also thank two reviewers for constructive criticism, Yann Vitasse for editing our submission, and Pekka Hirvonen (<ext-link ext-link-type="uri" xlink:href="http://www.toisinsanoen.eu">www.toisinsanoen.eu</ext-link>) for revising the language of the manuscript.</p>
</ack>
<sec id="S10" 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.2021.768963/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fpls.2021.768963/full#supplementary-material</ext-link></p>
<supplementary-material xlink:href="Data_Sheet_1.pdf" id="DS1" mimetype="application/pdf" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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