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<journal-id journal-id-type="publisher-id">Front. Plant Sci.</journal-id>
<journal-title-group>
<journal-title>Frontiers in Plant Science</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Plant Sci.</abbrev-journal-title>
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<issn pub-type="epub">1664-462X</issn>
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<publisher-name>Frontiers Media S.A.</publisher-name>
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<article-meta>
<article-id pub-id-type="doi">10.3389/fpls.2026.1745759</article-id>
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<subj-group subj-group-type="heading">
<subject>Original Research</subject>
</subj-group>
</article-categories>
<title-group>
<article-title>Study on physiological indicators and spectral response characteristics of alfalfa under simulated spontaneous combustion of coal gangue dumps</article-title>
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<contrib contrib-type="author">
<name><surname>He</surname><given-names>Meichen</given-names></name>
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<contrib contrib-type="author">
<name><surname>Ren</surname><given-names>He</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
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<contrib contrib-type="author" corresp="yes">
<name><surname>Zhao</surname><given-names>Yanling</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="corresp" rid="c001"><sup>*</sup></xref>
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<contrib contrib-type="author">
<name><surname>He</surname><given-names>Tingting</given-names></name>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
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<contrib contrib-type="author">
<name><surname>Chen</surname><given-names>Chunfang</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
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<name><surname>Zhang</surname><given-names>Lifan</given-names></name>
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<contrib contrib-type="author">
<name><surname>Tang</surname><given-names>Yanjie</given-names></name>
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<aff id="aff1"><label>1</label><institution>College of Geoscience and Surveying Engineering, China University of Mining and Technology</institution>, <city>Beijing</city>,&#xa0;<country country="cn">China</country></aff>
<aff id="aff2"><label>2</label><institution>Academy of Eco-Civilization Development for Jing-Jin-Ji Megalopolis, Tianjin Normal University</institution>, <city>Tianjin</city>,&#xa0;<country country="cn">China</country></aff>
<aff id="aff3"><label>3</label><institution>Advanced Laser Technology Laboratory of Anhui Province</institution>, <city>Hefei</city>,&#xa0;<country country="cn">China</country></aff>
<author-notes>
<corresp id="c001"><label>*</label>Correspondence: Yanling Zhao, <email xlink:href="mailto:ylzhao@cumtb.edu.cn">ylzhao@cumtb.edu.cn</email></corresp>
</author-notes>
<pub-date publication-format="electronic" date-type="pub" iso-8601-date="2026-02-04">
<day>04</day>
<month>02</month>
<year>2026</year>
</pub-date>
<pub-date publication-format="electronic" date-type="collection">
<year>2026</year>
</pub-date>
<volume>17</volume>
<elocation-id>1745759</elocation-id>
<history>
<date date-type="received">
<day>14</day>
<month>11</month>
<year>2025</year>
</date>
<date date-type="accepted">
<day>19</day>
<month>01</month>
<year>2026</year>
</date>
<date date-type="rev-recd">
<day>16</day>
<month>01</month>
<year>2026</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2026 He, Ren, Zhao, He, Chen, Zhang and Tang.</copyright-statement>
<copyright-year>2026</copyright-year>
<copyright-holder>He, Ren, Zhao, He, Chen, Zhang and Tang</copyright-holder>
<license>
<ali:license_ref start_date="2026-02-04">https://creativecommons.org/licenses/by/4.0/</ali:license_ref>
<license-p>This is an open-access article distributed under the terms of the <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">Creative Commons Attribution License (CC BY)</ext-link>. 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.</license-p>
</license>
</permissions>
<abstract>
<sec>
<title>Introduction</title>
<p>Coal gangue dumps may still pose a risk of spontaneous combustion even after reclamation, threatening both ecological restoration and surrounding environments. As a dynamic and complex process, vegetation responses to spontaneous combustion heat stress vary across growth stages. Therefore, identifying growth-stage-dependent spectral responses of physiological indicators is critical for the timely and accurate detection of spontaneous combustion in coal gangue dumps.</p>
</sec>
<sec>
<title>Methods</title>
<p>In contrast to field-based investigations, this study selected alfalfa (<italic>Medicago sativa</italic> L.), a typical reclaimed herbaceous species on coal gangue dumps, as the study object. Constant high-temperature conditions were established indoors to simulate heat stress associated with coal gangue spontaneous combustion. The spectral response differences of chlorophyll relative content (SPAD) and photosynthetic parameters at different growth stages were analyzed. Correlation analysis combined with the SPA algorithm was applied to identify sensitive physiological indicators, spectral bands, and characteristic parameters related to heat stress. Subsequently, support vector regression (SVR), random forest regression (RFR), and partial least squares regression (PLSR) models were developed (training set: test set = 3:1, n = 60:20) to determine optimal combinations of growth stage, indicators, and spectral features for monitoring spontaneous-combustion-induced heat stress.</p>
</sec>
<sec>
<title>Results</title>
<p>(1) during branching, budding, and flowering stages, the SPAD values and photosynthetic parameters of treatment (T) and control (CK) groups exhibited consistent trends; (2) sensitive features included OS2, FDS1, FDS2, TP, NDVI, and FDNDVI; and (3) vegetation indices based on original spectra achieved the highest prediction accuracy, followed by those derived from first-derivative spectra, triangular parameters, first-derivative reflectance, and original spectral bands. Among all growth stages, the budding stage was identified as the optimal observation period, and the SVR model showed the best performance (FDNDVI: R&#xb2; = 0.77, RMSE&#xa0;=&#xa0;3.50).</p>
</sec>
<sec>
<title>Discussion</title>
<p>This study reveals growth-stage-dependent physiological and spectral responses of vegetation to spontaneous combustion heat stress and provides a theoretical basis and technical reference for ecological monitoring and early warning of spontaneous combustion in reclaimed coal gangue dumps.</p>
</sec>
</abstract>
<kwd-group>
<kwd>alfalfa</kwd>
<kwd>coal gangue dumps</kwd>
<kwd>heat stress</kwd>
<kwd>model prediction</kwd>
<kwd>spectral response</kwd>
<kwd>spontaneous combustion</kwd>
</kwd-group>
<funding-group>
<funding-statement>The author(s) declared that financial support was received for this work and/or its publication. This study was supported by the financial support from the National Natural Science Foundation of China (No. 420701250 and No. 42507624).</funding-statement>
</funding-group>
<counts>
<fig-count count="8"/>
<table-count count="7"/>
<equation-count count="7"/>
<ref-count count="95"/>
<page-count count="21"/>
<word-count count="11129"/>
</counts>
<custom-meta-group>
<custom-meta>
<meta-name>section-at-acceptance</meta-name>
<meta-value>Plant Physiology</meta-value>
</custom-meta>
</custom-meta-group>
</article-meta>
</front>
<body>
<sec id="s1" sec-type="intro">
<label>1</label>
<title>Introduction</title>
<p>Coal gangue, as a primary waste product generated during coal mining and beneficiation processes, is currently one of the largest accumulated solid wastes in China (<xref ref-type="bibr" rid="B1">Abramowicz et&#xa0;al., 2021</xref>). Due to its low utilization efficiency, coal gangue are generally abandoned near mining sites, where they accumulate into large heaps (<xref ref-type="bibr" rid="B33">Li and Wang, 2019</xref>). Statistics indicate that there are currently over 2,600 large-scale coal gangue dumps in China, with a total accumulated volume exceeding 7 billion tons, occupying approximately 1.5 million km&#xb2; of land, and increasing at an annual rate of 300 million tons (<xref ref-type="bibr" rid="B58">Song et&#xa0;al., 2022</xref>). Certain components of coal gangue, including residual media, pyrite, sulfide minerals, and other organic substances, are highly prone to spontaneous combustion, releasing harmful gases such as CO and SO<sub>2</sub> as well as inhalable particulate matter into the atmosphere (<xref ref-type="bibr" rid="B31">Li et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B33">Li and Wang, 2019</xref>; <xref ref-type="bibr" rid="B86">Zhang et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B22">He et&#xa0;al., 2025</xref>). This poses a serious threat to the natural environment and human health. Furthermore, rainwater erosion can contaminate surrounding soils and groundwater, causing environmental pollution. Studies have shown that even when mining companies implement fire suppression measures and ecological restoration projects on spontaneously combusting coal gangue dumps, the restored dumps still face the risk of re-ignition (<xref ref-type="bibr" rid="B43">Ren et&#xa0;al., 2020</xref>, <xref ref-type="bibr" rid="B42">2023</xref>; <xref ref-type="bibr" rid="B45">Ren et&#xa0;al., 2022a</xref>). To prevent secondary ecological risks in reclaimed coal gangue dumps, early identification of spontaneous combustion is essential. Through the effective application of ecological restoration technologies and comprehensive management measures, maintaining the evergreen status of coal gangue dumps is of significant practical importance and long-term value for improving regional ecological environments.</p>
<p>Currently, the primary monitoring targets for spontaneous combustion in coal gangue dumps include surface temperature (<xref ref-type="bibr" rid="B2">Anghelescu and Diaconu, 2024</xref>; <xref ref-type="bibr" rid="B25">Jiang et&#xa0;al., 2023</xref>; <xref ref-type="bibr" rid="B32">Li et&#xa0;al., 2020</xref>; <xref ref-type="bibr" rid="B50">Shao et&#xa0;al., 2024</xref>; <xref ref-type="bibr" rid="B89">Zhao et&#xa0;al., 2023</xref>) and harmful gases (<xref ref-type="bibr" rid="B31">Li et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B49">Shao et&#xa0;al., 2023</xref>; <xref ref-type="bibr" rid="B90">Zhao et&#xa0;al., 2022</xref>). <xref ref-type="bibr" rid="B70">Wang et&#xa0;al. (2020)</xref> delineated high-temperature zones by integrating infrared thermal imaging, borehole temperature measurements, and radon concentration data, establishing a risk assessment method for coal gangue spontaneous combustion and analyzing gas toxicity, explosion hazards, and fire trends in construction areas (<xref ref-type="bibr" rid="B70">Wang et&#xa0;al., 2020</xref>). Zhao et&#xa0;al. (2022) monitored the temperature of coal gangue stockpiles using heat pipes and monitoring software, developed fitting models for shallow and deep temperatures, and analyzed internal temperature variations (<xref ref-type="bibr" rid="B90">Zhao et&#xa0;al., 2022</xref>). <xref ref-type="bibr" rid="B49">Shao et&#xa0;al. (2023)</xref> utilized UAV-based infrared oblique photogrammetry combined with custom software to construct 3D temperature models of coal gangue dumps (<xref ref-type="bibr" rid="B49">Shao et&#xa0;al., 2023</xref>). <xref ref-type="bibr" rid="B75">Wasilewski (2020)</xref> conducted long-term observations of thermal and gaseous activities in coal gangue dumps using thermal imaging cameras and fixed-point boreholes, developed and applied a numerical model based on initial boundary conditions and atmospheric parameters to identify features most likely to influence fire sources in spoil heaps, and proposed a modern method for monitoring fire hazards in coal mine spoil heaps (<xref ref-type="bibr" rid="B75">Wasilewski, 2020</xref>).</p>
<p>Vegetation growth is strongly influenced by the environment (<xref ref-type="bibr" rid="B64">Tauqeer et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B82">Yang et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B20">He et&#xa0;al., 2023</xref>), and monitoring vegetation growth status is therefore an effective approach for stress identification. <xref ref-type="bibr" rid="B26">Jin et&#xa0;al. (2023)</xref> identified drought stress by monitoring photosynthetic parameters, chlorophyll fluorescence parameters, and proline content in Sargent&#x2019;s cherry trees (<italic>Prunus sargentii</italic> Rehder) (<xref ref-type="bibr" rid="B26">Jin et&#xa0;al., 2023</xref>). Compared with the control group, the growth parameters of lettuce (<italic>Lactuca sativa</italic> L.) seedlings were significantly reduced under drought stress (<xref ref-type="bibr" rid="B55">Shin et&#xa0;al., 2021</xref>). <xref ref-type="bibr" rid="B23">Hu et&#xa0;al. (2025)</xref> conducted controlled water-stress experiments and found that one-year-old &#x201c;Suchazao&#x201d; tea plants exhibited different sensitive physiological indicators under different stress levels, which could serve as effective criteria for identifying varying degrees of water stress (<xref ref-type="bibr" rid="B23">Hu et&#xa0;al., 2025</xref>). High-temperature stress induced by spontaneous combustion in coal gangue dumps is the most prominent abiotic stress factor affecting vegetation growth and physiological functioning, and in severe cases it can even lead to open flames at the surface. Studies have shown that under high-temperature stress, plant cells perceive elevated temperatures through the plasma membrane, triggering Ca<sup>2+</sup> influx and subsequent binding with calmodulin, thereby initiating specific signal transduction pathways and activating heat stress response mechanisms (<xref ref-type="bibr" rid="B69">Wang et&#xa0;al., 2018</xref>). The phenotypic effects of high-temperature stress on plants are mainly manifested as leaf yellowing, wilting, and abscission, as well as reduced growth rates and overall dwarfing (<xref ref-type="bibr" rid="B51">Sharma et&#xa0;al., 2020</xref>). Meanwhile, high-temperature stress can cause cellular damage and disrupt physiological activities and hormonal regulation (<xref ref-type="bibr" rid="B10">Driedonks et&#xa0;al., 2015</xref>). Photosynthesis provides the energy and material basis for plant life activities. Vegetation exchanges CO<sub>2</sub>, water vapor, and other substances with the environment through stomata, and both photosynthesis and stomatal behavior are highly sensitive to environmental fluctuations. High-temperature stress significantly affects photosynthetic processes and stomatal regulation (<xref ref-type="bibr" rid="B62">Sun et&#xa0;al., 2023</xref>; <xref ref-type="bibr" rid="B71">Wang et&#xa0;al., 2025</xref>; <xref ref-type="bibr" rid="B79">Xu, 1988</xref>), while also altering physiological parameters closely associated with photosynthesis, such as the contents of photosynthetic pigments including chlorophyll. Under high-temperature stress, azalea exhibits reduced chlorophyll fluorescence, decreased stomatal characteristics, and a decline in photosynthetic rate (<xref ref-type="bibr" rid="B27">Khan et&#xa0;al., 2025</xref>). Vicente et&#xa0;al. reported that temperature variations influence vessel structure, stomatal dynamics, and assimilation capacity of European beech (Fagus sylvatica) in the southern Alps (<xref ref-type="bibr" rid="B65">Vicente et&#xa0;al., 2022</xref>). Feng et&#xa0;al. demonstrated that temperature changes significantly affect the photosynthetic characteristics and flowering performance of two Paphiopedilum species in southwestern China (<xref ref-type="bibr" rid="B13">Feng et&#xa0;al., 2022</xref>). High-temperature stress (HS) increased canopy temperature (CT), the chlorophyll a/b ratio, leaf wax content, and anthocyanin content in pea plants, while significantly decreasing the contents of chlorophyll a, chlorophyll b, and carotenoids (<xref ref-type="bibr" rid="B63">Tafesse, 2018</xref>). Changes in photosynthetic pigment contents indirectly alter vegetation spectral characteristics, thereby providing a basis for monitoring and quantifying vegetation heat stress using hyperspectral techniques.</p>
<p>When vegetation is subjected to stress, physiological indicators change accordingly, and these changes further influence spectral responses. Spectral analysis can therefore be used to assess vegetation growth status (<xref ref-type="bibr" rid="B29">Kothari and Schweiger, 2022</xref>; <xref ref-type="bibr" rid="B46">Ren et&#xa0;al., 2020b</xref>). Hyperspectral techniques enable accurate estimation of vegetation growth information, and the response relationships between physiological indicators and spectral characteristics can reveal the spectral representation mechanisms underlying physiological changes in vegetation (<xref ref-type="bibr" rid="B44">Ren et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B74">Wang et&#xa0;al., 2021</xref>). At present, commonly used methods for spectral feature extraction include Principal Component Analysis (PCA), Maximum Noise Fraction (MNF), Linear Discriminant Analysis (LDA), Discrete Wavelet Transform (DWT), and Independent Component Analysis (ICA) (<xref ref-type="bibr" rid="B6">Benoit et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B17">Guo et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B30">Lan et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B38">Othman and Zeebaree, 2020</xref>; <xref ref-type="bibr" rid="B91">Zhao et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B92">Zhu et&#xa0;al., 2022</xref>). Band selection methods mainly include Competitive Adaptive Reweighted Sampling (CARS), Uninformative Variable Elimination (UVE), and the Successive Projection Algorithm (SPA) (<xref ref-type="bibr" rid="B57">Song et&#xa0;al., 2020</xref>; <xref ref-type="bibr" rid="B81">Yan et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B83">Yao et&#xa0;al., 2022</xref>). Frequently used modeling approaches include Support Vector Machine (SVM), Random Forest (RF), Multiple Linear Regression (MLR), and Partial Least Squares (PLS) (<xref ref-type="bibr" rid="B7">Cervantes et&#xa0;al., 2020</xref>; <xref ref-type="bibr" rid="B52">Shen et&#xa0;al., 2020</xref>; <xref ref-type="bibr" rid="B56">Singh et&#xa0;al., 2024</xref>; <xref ref-type="bibr" rid="B60">Sun et&#xa0;al., 2020</xref>). <xref ref-type="bibr" rid="B88">Zhang et&#xa0;al. (2025)</xref> conducted experiments on maize under different Cu<sup>2+</sup> concentrations and applied second-order derivative (SOD) processing and continuum removal (CR) to leaf spectral reflectance. Combined with the leaf spectral detection method (LSDN), spectral information was enhanced, enabling the localization of abnormal spectral bands. The extracted spectral anomaly parameters quantitatively characterized maize leaf abnormalities under copper stress (<xref ref-type="bibr" rid="B88">Zhang et&#xa0;al., 2025</xref>). <xref ref-type="bibr" rid="B15">Gu et&#xa0;al. (2026)</xref> proposed an Extreme Gradient Boosting (XGBoost) model optimized using the Sparrow Search Algorithm (SSA) and an Extreme Learning Machine (ELM) model optimized with the Artificial Hummingbird Algorithm (AHA), both of which demonstrated superior performance in predicting wheat leaf nitrogen content (LNC) (<xref ref-type="bibr" rid="B15">Gu et&#xa0;al., 2026</xref>).</p>
<p>Heat stress induced by spontaneous combustion in coal gangue dumps has a significant impact on vegetation. The spontaneous combustion process affects soil pH and nutrient composition, which indirectly influences plant growth status, community composition, and ecological functions (<xref ref-type="bibr" rid="B41">Ran et&#xa0;al., 2020</xref>; <xref ref-type="bibr" rid="B48">Ruan et&#xa0;al., 2022</xref>). Numerous scholars have indicated that changes in vegetation physiological status serve as indirect indicators of combustion risk, representing an effective monitoring approach (<xref ref-type="bibr" rid="B11">Du and Zhang, 2009</xref>; <xref ref-type="bibr" rid="B84">Zhang, 2008</xref>). Researchers in Poland have identified a &#x201c;natural greenhouse effect&#x201d; on coal gangue dumps, characterized by the persistence of alternating vegetation during winter. Additionally, they observed plants with heights significantly exceeding historical records, potentially related to increased nitrogen availability, soil temperature, and carbon dioxide concentration (<xref ref-type="bibr" rid="B9">Ciesielczuk et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B59">Stracher et&#xa0;al., 2015</xref>). Field investigations revealed that alfalfa (<italic>Medicago sativa</italic> L.) is widely distributed across coal gangue dumps and is the dominant herbaceous species in both spontaneous combustion zones and vegetated areas. Under coal gangue dump conditions, alfalfa persists for most of the year (<xref ref-type="bibr" rid="B93">Zhu et&#xa0;al., 2021</xref>), demonstrating strong adaptability to the coal gangue environment. Under heat stress induced by spontaneous combustion, alfalfa exhibits pronounced variations in vegetation traits. In a spontaneous combustion area of a coal gangue dump in Shanxi Province, alfalfa biomass decreased by more than 300&#xa0;g m<sup>-2</sup> and plant height declined by over 30&#xa0;cm compared with plants in unaffected areas. From the combustion zone to the safe zone, alfalfa showed significant spatial variation: the closer to the combustion zone, the larger the yellowing area at the roots, whereas alfalfa in safe zones exhibited a healthy green appearance (<xref ref-type="bibr" rid="B45">Ren et&#xa0;al., 2022a</xref>; <xref ref-type="bibr" rid="B46">Ren et&#xa0;al., 2022b</xref>). <xref ref-type="bibr" rid="B74">Wang et&#xa0;al. (2021</xref>, <xref ref-type="bibr" rid="B73">2022a)</xref> conducted indoor simulation experiments to reproduce high-temperature environments associated with spontaneous combustion in coal gangue dumps and investigated heat stress effects on alfalfa. At both leaf and canopy scales, vegetation indices, correlation analysis, Lasso regression, and long short-term memory (LSTM) networks were applied. Through time-series analysis and feature selection, optimal spectral bands and vegetation indices were identified, and an SF-LSTM model was developed to discriminate heat stress intensity. The results indicated differences in sensitive bands between first-derivative spectra and original spectra, and heat stress was classified into mild, moderate, and severe levels based on stress symptoms. Furthermore, quantitative relationships between physiological indicators and spectral responses were established using alfalfa water content and fluorescence parameters (<xref ref-type="bibr" rid="B74">Wang et&#xa0;al., 2021</xref>, <xref ref-type="bibr" rid="B73">2022</xref>). <xref ref-type="bibr" rid="B45">Ren et&#xa0;al. (2022a)</xref> and <xref ref-type="bibr" rid="B46">Ren et&#xa0;al. (2022b)</xref> combined unmanned aerial vehicle (UAV) imagery with field survey data and successfully estimated aboveground biomass (AGB) and plant height (PH) of alfalfa using UAV-derived red-edge chlorophyll index (CIrededge), canopy temperature depression (CTD), and canopy height model (CHM). Based on vegetation phenotypic parameters, a subsurface spontaneous combustion indication model was developed, enabling the quantification of the spatial distribution of spontaneous combustion intensity in coal gangue dumps (<xref ref-type="bibr" rid="B46">Ren et&#xa0;al., 2022b</xref>).</p>
<p>However, spontaneous combustion in coal gangue dumps is a complex and dynamic process, and alfalfa experiences different combustion stages throughout its life cycle. Physiological indicators and spectral responses of alfalfa vary across growth stages under spontaneous-combustion-induced heat stress. Existing studies have largely focused on vegetation physiological status at the whole life-cycle scale, with limited attention to differences in physiological states and spectral response characteristics among individual growth stages. Comparing growth-stage-dependent responses and identifying sensitive growth stages, physiological traits, and spectral features indicative of spontaneous combustion are therefore essential for improving the foundation and diagnostic capability of coal gangue dump spontaneous combustion monitoring.</p>
<p>To address this issue, this study selected alfalfa (<italic>Medicago sativa</italic>&#xa0;L.), a typical perennial herbaceous species used for reclamation on coal gangue dumps, as the research object. An indoor constant-temperature experiment was conducted to simulate heat stress during the early stage of spontaneous combustion in coal gangue dumps by establishing a control group and a warming treatment group. The effects of heat stress on alfalfa were analyzed based on physiological indicators, including SPAD and photosynthetic parameters, as well as canopy-level spectral characteristics. The main objectives of this study were to: (1) analyze the spectral response characteristics of alfalfa under heat stress induced by spontaneous combustion in coal gangue dumps and identify spectral bands and characteristic parameters sensitive to heat stress at different growth stages; (2) investigate the response relationships between key physiological parameters of alfalfa and spectral features to clarify the physiological mechanisms underlying spectral changes; and (3) construct and optimize spectral prediction models for monitoring heat stress in alfalfa based on sensitive spectral features, with the aim of providing technical support for the monitoring and early warning of spontaneous combustion in reclaimed coal gangue dumps.</p>
</sec>
<sec id="s2" sec-type="materials|methods">
<label>2</label>
<title>Material and methods</title>
<sec id="s2_1">
<label>2.1</label>
<title>Experimental design and data acquisition</title>
<sec id="s2_1_1">
<label>2.1.1</label>
<title>Experimental design</title>
<p>The experiment was conducted from April to July 2022 using a potted cultivation approach. Alfalfa was planted in plastic pots with a bottom diameter of 18&#xa0;cm, a top diameter of 28&#xa0;cm, and a height of 31.5&#xa0;cm. The experimental soil consisted of a mixture of 17.5&#xa0;kg of general garden soil and 0.5&#xa0;kg of nutrient soil per pot. Compound fertilizer (with approximately 15%-15%-15% nitrogen-phosphorus-potassium content) was applied at a rate of 2.5&#xa0;g per pot during the branching and budding stages.</p>
<p>Alfalfa, a commonly used perennial herbaceous species for ecological restoration on coal gangue dumps, was selected for this study. The variety used was the imported &#x2018;<italic>Medicago sativa</italic> L.&#x2019;. The experiment included one control group (CK) and one treatment group (T), each with four replicates. The control group was allowed to grow naturally, while the treatment group was subjected to a heat source of 120&#xa0;&#xb0;C applied 30&#xa0;cm deep in the soil to simulate the temperature stress generated during spontaneous combustion of coal gangue dumps (<xref ref-type="fig" rid="f1"><bold>Figure&#xa0;1</bold></xref>). Soils on coal gangue dumps are highly heterogeneous and involve numerous confounding factors, such as variations in heavy metal contents and microbial communities. In addition, coal gangue dumps are typically covered with a soil layer of 30&#x2013;50 cm and have already undergone ecological restoration. Conducting indoor experiments would require a large quantity of soil, and directly collecting soil samples from coal gangue dumps would cause substantial disturbance to the local ecosystem and seriously compromise restoration efforts. Therefore, homogeneous soil was used in this study.</p>
<fig id="f1" position="float">
<label>Figure&#xa0;1</label>
<caption>
<p>Schematic diagram of experimental design.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-17-1745759-g001.tif">
<alt-text content-type="machine-generated">Diagram showing a container with dimensions 28 centimeters wide, 31.5 centimeters tall, and 18 centimeters at the base. A heating pad is depicted at the bottom, connected to a temperature controller. Insets compare plant growth under room temperature (Group CK) and heat stress (Group T), with plant growth differences shown.</alt-text>
</graphic></fig>
<p>Alfalfa was sown on April 16, 2022. Prior to sowing, uniform and full alfalfa seeds were selected, with 0.26&#xa0;g sown per pot. One week after emergence of approximately half the seedlings, thinning was conducted to maintain 60 plants per pot before heat treatment. Each pot was watered with 0.5 L daily, with an additional 0.25 L applied during hot weather to ensure adequate moisture. Indoor temperature was controlled between 24&#xa0;&#xb0;C and 27&#xa0;&#xb0;C. Data were collected at intervals of four days; depending on weather conditions, measurements were advanced or delayed by one day, maintaining a final data collection interval of 3&#x2013;5 days. A total of 14 measurements were conducted, all of which were completed in 2022. Specifically, measurements were carried out on May 22, May 26, June 1, June 5, and June 10, during which alfalfa was at the branching stage. Subsequent measurements were performed on June 14, June 18, June 23, June 26, and June 30, corresponding to the budding stage of alfalfa. Finally, measurements conducted on July 5, July 9, July 14, and July 18 captured the flowering stage of alfalfa.</p>
</sec>
<sec id="s2_1_2">
<label>2.1.2</label>
<title>Data acquisition</title>
<p>SPAD values were measured using a SPAD-502 portable chlorophyll meter. Two pots were selected per group for measurement. Within each pot, a five-point measurement method was applied, randomly selecting the second and third fully expanded leaves from 10 uniformly growing plants as samples. As the growth stage progressed, leaves 1 and 2 from the lower part of the third fully expanded leaf were selected in later stages. Each individual leaf was measured five times, and the average value was recorded.</p>
<p>Photosynthetic and fluorescence parameters were measured using the LI-6800 portable photosynthesis system between 8:30 AM and 11:30 AM. After instrument calibration, environmental parameters were set for measurement (ambient CO<sub>2</sub> concentration set at 400 &#xb5;mol mol<sup>-1</sup>, temperature adjusted to 25&#xa0;&#xb0;C, humidity at 55%, fan speed at 10,000 rpm, and airflow rate at a conventional 500&#xa0;&#xb5;mol s<sup>-1</sup>). The leaf chamber was set to a semi-open and semi-closed state, with leaves clamped inside for measurement. Gas exchange parameters obtained included photosynthetic rate (A, &#xb5;mol m<sup>-2</sup> s<sup>-1</sup>), intercellular CO<sub>2</sub> concentration (Ci, &#xb5;mol mol<sup>-1</sup>), and stomatal conductance (gsw, mol m<sup>-2</sup> s<sup>-1</sup>). Fluorescence parameters mainly included the effective quantum yield of PSII under light (<inline-formula>
<mml:math display="inline" id="im1"><mml:mrow><mml:mtext>Fv'</mml:mtext><mml:mo stretchy="false">/</mml:mo><mml:mtext>Fm'</mml:mtext></mml:mrow></mml:math></inline-formula>), photochemical quenching coefficient (qP), and non-photochemical quenching coefficient (qN).</p>
<p>Canopy spectra were measured using an SVC HR-1024i full-range field spectrometer, with detailed technical specifications shown in <xref ref-type="table" rid="T1"><bold>Table&#xa0;1</bold></xref>. Measurements were conducted on clear and windless days between 11:00 a.m. and 2:00 p.m. Two pots per group were measured, with white reference calibration performed before each measurement. Each pot was measured using the five-point method, and each sample was measured three times; the mean value was recorded as the alfalfa canopy spectral data, covering the spectral range from 350 to 1350 nm.</p>
<table-wrap id="T1" position="float">
<label>Table&#xa0;1</label>
<caption>
<p>SVC HR-10241 technical specifications of high-resolution full-spectrum field spectrometer.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" align="center">Parameter</th>
<th valign="middle" align="center">Specification</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="center">Weight</td>
<td valign="middle" align="center">3.8kg</td>
</tr>
<tr>
<td valign="middle" align="center">Spectral Range</td>
<td valign="middle" align="center">350nm~2500nm</td>
</tr>
<tr>
<td valign="middle" align="center">Spectral Resolution</td>
<td valign="middle" align="center">&#x2264;3.5nm@700nm &#x2264;9.5nm@1500nm &#x2264;6.5nm@2100nm</td>
</tr>
<tr>
<td valign="middle" align="center">Spectral Sampling Width</td>
<td valign="middle" align="center">1.5nm, 350-1000 3.8nm, 1000-1885 2.5nm, 1885-2500</td>
</tr>
<tr>
<td valign="middle" align="center">Field of View</td>
<td valign="middle" align="center">Lens:4&#xb0; Optical Fiber:25&#xb0;</td>
</tr>
<tr>
<td valign="middle" align="center">Wavelength Accuracy</td>
<td valign="middle" align="center">0.5nm</td>
</tr>
<tr>
<td valign="middle" align="center">Wavelength Repeatability</td>
<td valign="middle" align="center">0.1nm</td>
</tr>
<tr>
<td valign="middle" align="center">Operating Environment</td>
<td valign="middle" align="center">Temperature;-10&#xb0;C~40&#xb0;C Humidity:&lt;90% Non-condensing</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>To reduce interference, spectral data were preprocessed using the accompanying SVC HR-1024i software. Data were first de-duplicated, then resampled, followed by smoothing of spectral curves using the Savitzky-Golay convolution smoothing method.</p>
<p>Data analysis and correlation analysis were conducted using Origin 2021. In addition, Origin 2021 was used to generate graphical outputs of the analytical results, and figure integration and layout were completed using Microsoft PowerPoint 2019.</p>
</sec>
</sec>
<sec id="s2_2">
<label>2.2</label>
<title>Methods</title>
<sec id="s2_2_1">
<label>2.2.1</label>
<title>Extraction of sensitive spectral bands</title>
<p>This study employed correlation analysis to select sensitive spectral bands of alfalfa physiological indicators. Using the original spectral reflectance (R) and its first derivative reflectance (FDR) in the 350&#x2013;1350 nm range as independent variables, and physiological indicators such as chlorophyll content (SPAD) and photosynthetic parameters as dependent variables. Based on <xref ref-type="disp-formula" rid="eq1">Equation (1)</xref>, the Pearson correlation coefficient was calculated for each wavelength band:</p>
<disp-formula id="eq1"><label>(1)</label>
<mml:math display="block" id="M1"><mml:mrow><mml:mi>r</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>&#x3bb;</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msubsup><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:msubsup><mml:mo stretchy="false">(</mml:mo><mml:mi>R</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>&#x3bb;</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo stretchy="false">)</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mi>R</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>&#x2212;</mml:mo><mml:mi>Y</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:msqrt><mml:mrow><mml:msubsup><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:msubsup><mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mi>R</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>&#x3bb;</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo stretchy="false">)</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mover accent="true"><mml:mi>R</mml:mi><mml:mo>&#xaf;</mml:mo></mml:mover><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msup><mml:msubsup><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:msubsup><mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>Y</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>&#x2212;</mml:mo><mml:mover accent="true"><mml:mi>Y</mml:mi><mml:mo>&#xaf;</mml:mo></mml:mover><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msup></mml:mrow></mml:msqrt></mml:mrow></mml:mfrac></mml:mrow></mml:math>
</disp-formula>
<p>Where <inline-formula>
<mml:math display="inline" id="im2"><mml:mrow><mml:msub><mml:mi>Y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> represents the measured physiological indicator value and <inline-formula>
<mml:math display="inline" id="im3"><mml:mrow><mml:msub><mml:mi>&#x3bb;</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> denotes the wavelength value.</p>
<p>To reduce redundancy among spectral bands and minimize the influence of measurement environment, the original and first derivative spectra in the 350&#x2013;1350 nm range were used as independent variables, with physiological indicator measurements as dependent variables. Correlation analysis combined with SPA was applied to select characteristic spectral bands sensitive to physiological indicators, i.e., bands that had significant influence on physiological parameters. In this study, SPA modeling used 40 samples for calibration and 40 for prediction, resulting in the selection of different spectral feature bands for the branching stage.</p>
<p>SPA is a forward iterative search method that starts from one wavelength and adds a new wavelength at each iteration until the preset number of variables is reached. The goal of SPA is to select a wavelength combination with minimal redundancy in spectral information to address collinearity issues (<xref ref-type="bibr" rid="B3">Ara&#xfa;jo et&#xa0;al., 2001</xref>; <xref ref-type="bibr" rid="B37">Mu et&#xa0;al., 2014</xref>). SPA was calculated based on <xref ref-type="disp-formula" rid="eq2">Equations 2</xref>&#x2013;<xref ref-type="disp-formula" rid="eq4">4</xref>. The input includes the spectral data X. Initial band set K(0), the preset number of variables N, initialized iteration n=1, and spectral variables <inline-formula>
<mml:math display="inline" id="im4"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>&#x2208;</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, j=1, &#x2026;J.</p>
<p>1) Identification of unselected wavelength variables:</p>
<disp-formula id="eq2"><label>(2)</label>
<mml:math display="block" id="M2"><mml:mrow><mml:mi>S</mml:mi><mml:mo>=</mml:mo><mml:mo>{</mml:mo><mml:mi>j</mml:mi><mml:mo>|</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x2264;</mml:mo><mml:mi>j</mml:mi><mml:mo>&#x2264;</mml:mo><mml:mi>J</mml:mi><mml:mo>&#xa0;</mml:mo><mml:mi>a</mml:mi><mml:mi>n</mml:mi><mml:mi>d</mml:mi><mml:mo>&#xa0;</mml:mo><mml:mi>j</mml:mi><mml:mo>&#x2209;</mml:mo><mml:mo>{</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>0</mml:mn><mml:mo stretchy="false">)</mml:mo><mml:mo>,</mml:mo><mml:mo>.</mml:mo><mml:mo>,</mml:mo><mml:mi>k</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo><mml:mo>}</mml:mo><mml:mi>}</mml:mi></mml:mrow></mml:math>
</disp-formula>
<p>2) Calculate the projection of each x<sub>j</sub> onto the residual vector:</p>
<disp-formula id="eq3"><label>(3)</label>
<mml:math display="block" id="M3"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>&#x2212;</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>X</mml:mi><mml:mi>j</mml:mi><mml:mi>T</mml:mi></mml:msubsup><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub><mml:mo stretchy="false">)</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub><mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi>X</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mi>T</mml:mi></mml:msubsup><mml:mo>&#x2212;</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msub><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>
</disp-formula>
<p>3) For all j <inline-formula>
<mml:math display="inline" id="im5"><mml:mrow><mml:mo>&#x2208;</mml:mo><mml:mi>S</mml:mi></mml:mrow></mml:math></inline-formula>,</p>
<disp-formula id="eq4"><label>(4)</label>
<mml:math display="block" id="M4"><mml:mrow><mml:mi>k</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>n</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>=</mml:mo><mml:mi>a</mml:mi><mml:mi>r</mml:mi><mml:mi>g</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>max</mml:mi><mml:mo>&#x2225;</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>&#x2225;</mml:mo><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo>&#x2208;</mml:mo><mml:mi>S</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math>
</disp-formula>
<p>4) <inline-formula>
<mml:math display="inline" id="im6"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>j</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mo>&#xa0;</mml:mo><mml:mi>j</mml:mi><mml:mo>&#x2208;</mml:mo><mml:mi>S</mml:mi></mml:mrow></mml:math></inline-formula>.</p>
<p>5) Increment n=n+1. If n&lt;N, return to step 1). The final variable set is denoted as s<sub>1</sub>={x<sub>k(n)</sub>|n=0,&#x2026;,N-1}.</p>
<p>For each iteration of k(0) and N, a multiple linear regression model is established to obtain the modeling set RMSECV. The optimal values of k(0) and N correspond to the minimum RMSECV.</p>
</sec>
<sec id="s2_2_2">
<label>2.2.2</label>
<title>Model prediction</title>
<p>Spectral features with strong correlation were selected from the original spectrum (OS), first derivative spectrum (FDS), triangular spectral parameters (TP), and vegetation indices (VI) as inputs for model development. Specifically, OS1 and FDS1 denote the top ten wavelength bands selected by correlation analysis from the original and first derivative spectra, while OS2 and FDS2 represent bands optimized by the SPA algorithm. For TP, indices with correlation coefficients above 0.6 were chosen (<xref ref-type="bibr" rid="B39">Phaneendra Kumar et&#xa0;al., 2024</xref>). VI was divided into two categories, with NDVI and FDNDVI serving as the optimal indices for the original and first derivative spectra, respectively. The dataset was divided into training and testing sets at a 3:1 ratio (60 training samples, 20 testing samples).</p>
<p>Three machine learning algorithms were applied for validation: Support Vector Regression (SVR), Random Forest Regression (RFR), and Partial Least Squares Regression (PLSR). SVR, an extension of support vector machines for nonlinear regression, balances approximation accuracy and model complexity, showing particular strength with small sample sizes and nonlinear data (<xref ref-type="bibr" rid="B72">Wang et&#xa0;al., 2023</xref>). RFR employs the Bagging technique within an ensemble of regression trees, demonstrating robustness to noise and outliers and reducing overfitting (<xref ref-type="bibr" rid="B61">Sun et&#xa0;al., 2022</xref>). PLSR combines multiple linear regression, principal component analysis, and canonical correlation analysis, excelling with limited samples by extracting richer information than classical regression methods (<xref ref-type="bibr" rid="B76">Wold et&#xa0;al., 2001</xref>).</p>
<p>The model calculations in this study were performed in the MATLAB R2019b environment. The kernel function of the SVR model was the radial basis function (RBF), with the penalty parameter and kernel gamma value optimized automatically by the model. The SVM function type was set to &#x3f5;-SVR, with a loss function parameter &#x3f5;=0.01. For the Random Forest Regression (RFR) model, the decision tree algorithm employed TreeBagger with 200 trees and a minimum leaf size of 5; the algorithm type was set to regression. Variables were randomly divided into training and testing sets at a ratio of 3:1.</p>
<p>Model performance was evaluated using the coefficient of determination (R<sup>2</sup>) and root mean square error (RMSE). A higher R<sup>2</sup> and lower RMSE indicate better predictive accuracy. The calculation formulas for these metrics are as follows:</p>
<disp-formula id="eq5"><label>(5)</label>
<mml:math display="block" id="M5"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn>2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mfrac><mml:mrow><mml:msubsup><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:msubsup><mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>&#x2212;</mml:mo><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="true">^</mml:mo></mml:mover><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msup></mml:mrow><mml:mrow><mml:msubsup><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:msubsup><mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>&#x2212;</mml:mo><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo>&#xaf;</mml:mo></mml:mover><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mrow></mml:math>
</disp-formula>
<disp-formula id="eq6"><label>(6)</label>
<mml:math display="block" id="M6"><mml:mrow><mml:mi>R</mml:mi><mml:mi>M</mml:mi><mml:mi>S</mml:mi><mml:mi>E</mml:mi><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:mfrac><mml:mn>1</mml:mn><mml:mi>N</mml:mi></mml:mfrac><mml:mstyle displaystyle="true"><mml:msubsup><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:msubsup><mml:mrow><mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>&#x2212;</mml:mo><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="true">&#xaf;</mml:mo></mml:mover><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msup></mml:mrow></mml:mstyle></mml:mrow></mml:msqrt></mml:mrow></mml:math>
</disp-formula>
<p>Where N is the number of samples, <inline-formula>
<mml:math display="inline" id="im7"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the actual value of the i-th sample, <inline-formula>
<mml:math display="inline" id="im8"><mml:mrow><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mo stretchy="true">&#xaf;</mml:mo></mml:mover></mml:mrow></mml:math></inline-formula> is the predicted value of the i-th sample, and <inline-formula>
<mml:math display="inline" id="im9"><mml:mover accent="true"><mml:mi>y</mml:mi><mml:mo>&#xaf;</mml:mo></mml:mover></mml:math></inline-formula>&#x200b; is the mean of the actual values of all samples.</p>
</sec>
</sec>
</sec>
<sec id="s3" sec-type="results">
<label>3</label>
<title>Results</title>
<sec id="s3_1">
<label>3.1</label>
<title>Canopy spectral and physiological variations under heat stress</title>
<sec id="s3_1_1">
<label>3.1.1</label>
<title>Canopy spectral changes</title>
<p>The canopy spectra of alfalfa during the branching, budding, and flowering stages are shown in <xref ref-type="fig" rid="f2"><bold>Figure&#xa0;2</bold></xref>. During the branching stage, the spectral reflectance in the visible band showed no significant difference between T and CK, but in the near-infrared (NIR) band, the reflectance of T was significantly higher than that of CK. At the budding stage, T exhibited higher reflectance than CK in the visible band, with an even more pronounced difference in the NIR band. During the flowering stage, the reflectance difference between the two groups across the full spectral range was relatively small; however, T still demonstrated higher reflectance in the NIR band. These observations indicated that heating treatment induced a marked spectral response in alfalfa growth, with the effect gradually weakening over time.</p>
<fig id="f2" position="float">
<label>Figure&#xa0;2</label>
<caption>
<p>Canopy spectral variations at different growth stages (<bold>(a)</bold> depicted the spectral comparisons of alfalfa at different growth stages under various treatments, while <bold>(b)</bold> illustrated the spectral comparisons of different growth stages within the same treatment group).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-17-1745759-g002.tif">
<alt-text content-type="machine-generated">Charts showing reflectance across different wavelengths at various growth stages. Chart (a) compares the branching, budding, and flowering stages for CK (solid line) and T (dashed line). Chart (b) displays these stages' reflectance patterns separately, using distinct line styles for CK and T. Reflectance values range from 0 to 0.8.</alt-text>
</graphic></fig>
<p>From a longitudinal comparison of spectral changes within the same treatment group across different stages, spectral reflectance of CK in the visible band exhibited a &#x201c;decrease followed by an increase&#x201d; trend, while the NIR plateau reflectance gradually increased. This suggests that the spectral characteristics of alfalfa vary significantly along its growth stages under natural conditions. In contrast, spectral reflectance of T in the visible band showed an &#x201c;increase followed by a decrease&#x201d; trend, while the NIR plateau also gradually increased. In the visible band, the green valley depth of T was notably greater than that of CK, indicating that heat stress affected chlorophyll absorption capacity. In the NIR plateau region, reflectance of T during the branching stage was significantly lower than during the budding and flowering stages, with relatively minor differences between the latter two stages. This pattern suggests that the initial increase in spectral reflectance induced by heat stress was pronounced, but as the stress duration extended, the vegetation gradually adapted and reflectance changes stabilized.</p>
<p>As shown in <xref ref-type="fig" rid="f3"><bold>Figure&#xa0;3</bold></xref>, the first derivative of the canopy spectra exhibited the greatest fluctuations within the red edge region (680&#xa0;nm&#x2013;780 nm), with the maximum values in T exceeding those in CK across all three growth stages. The red edge area in T was significantly larger than that in CK during all stages. During the branching stage, the red edge position for CK was at 725 nm, while T showed a red shift to 726 nm. At the budding stage, red edge position of CK shifted to 729 nm, whereas T exhibited a blue shift to 727 nm. During the flowering stage, red edge of CK was at 721 nm, and T showed a pronounced red shift to 728 nm. Within the same treatment group, red edge position of CK changed from an initial red shift to a subsequent blue shift, which is consistent with normal plant growth patterns. The red edge amplitude followed the order: budding stage &gt; flowering stage &gt; branching stage, while the red edge area ranked flowering stage &gt; budding stage &gt; branching stage. Red edge position of T also shifted from red to blue, with the red edge amplitude and area ranking as budding stage &gt; flowering stage &gt; branching stage. The effects of heat stress on the first derivative spectral changes in alfalfa showed no significant difference between the budding and flowering stages.</p>
<fig id="f3" position="float">
<label>Figure&#xa0;3</label>
<caption>
<p>First derivative changes of canopy spectra at different growth stages (<bold>a, c, e</bold> represent the branching, budding, and flowering stages, respectively; <bold>b, d, f</bold> correspond to the respective red edge profiles; <bold>A</bold> denotes CK, <bold>C</bold> denotes T, and <bold>B</bold> and <bold>D</bold> correspond to the red edge profiles).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-17-1745759-g003.tif">
<alt-text content-type="machine-generated">This image displays eight spectral reflectance graphs labeled a to f and A to D. Graphs a, c, and e plot wavelength against reflectance for CK and T conditions. Graphs b, d, and f focus on a narrower wavelength range. Graphs A, C, and E compare reflectance across branching, budding, and flowering stages, with graph B showing detailed reflectance for these stages in a specific range. Dashed and solid lines indicate different variables or conditions across the graphs.</alt-text>
</graphic></fig>
</sec>
<sec id="s3_1_2">
<label>3.1.2</label>
<title>Physiological parameter changes</title>
<p>The amplitude of variation was calculated using <xref ref-type="disp-formula" rid="eq7">Equation 7</xref>:</p>
<disp-formula id="eq7"><label>(7)</label>
<mml:math display="block" id="M7"><mml:mrow><mml:mi>&#x3b7;</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mo stretchy="false">[</mml:mo><mml:mi>V</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>T</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mi>V</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>C</mml:mi><mml:mi>K</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mo stretchy="false">]</mml:mo></mml:mrow><mml:mrow><mml:mi>V</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>C</mml:mi><mml:mi>K</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mfrac><mml:mo>*</mml:mo><mml:mn>100</mml:mn><mml:mo>%</mml:mo></mml:mrow></mml:math>
</disp-formula>
<p>As shown in <xref ref-type="fig" rid="f4"><bold>Figures&#xa0;4a&#x2013;c</bold></xref>, except for an amplitude increase of 0.65% on May 22, the variation amplitude of chlorophyll content (SPAD) in T was consistently lower than that in CK during the branching, budding, and flowering stages, with all exhibiting an increasing trend. In <xref ref-type="fig" rid="f4"><bold>Figure&#xa0;4d</bold></xref>, the overall trend across the three growth stages shows an initial increase followed by a decrease, indicating that the plant growth pattern remained unchanged. Comparing SPAD between CK and T, the amplitude of variation in T was lower at each stage, suggesting that heat stress exerted an inhibitory effect on the relative chlorophyll content. It can be inferred that temperature partially limits alfalfa growth. Furthermore, in <xref ref-type="fig" rid="f4"><bold>Figures&#xa0;4a&#x2013;c</bold></xref>, SPAD increments exhibited a pattern of first rising and then falling, with increase of CK generally exceeding that of T, indicating that heat stress restricted the rate of SPAD increase to some extent.</p>
<fig id="f4" position="float">
<label>Figure&#xa0;4</label>
<caption>
<p>SPAD variation trends at different growth stages (<bold>(a)</bold> branching stage <bold>(b)</bold> budding stage <bold>(c)</bold> flowering stage <bold>(d)</bold> changes across all three stages).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-17-1745759-g004.tif">
<alt-text content-type="machine-generated">Bar charts comparing SPAD values between CK and T groups at various dates and growth stages. Charts (a), (b), and (c) show SPAD readings for specific dates while chart (d) displays values across growth stages: branching, budding, and flowering. CK consistently shows higher or similar SPAD values compared to T. Error bars indicate variability.</alt-text>
</graphic></fig>
<p>As shown in <xref ref-type="fig" rid="f5"><bold>Figure&#xa0;5</bold></xref>, the photosynthetic rate (A) variation trend in T was generally consistent with that of CK. Except during the branching stage, where the amplitude of change in T exceeded that of CK, the variation amplitudes on other dates were all lower than those in CK. During the branching stage, photosynthetic rate of T initially increased and then decreased; in the budding stage, it first increased, then decreased, and increased again; during the flowering stage, it rose initially and then declined. Overall, the photosynthetic rate decreased by 3.32%, 25.17%, and 17.46% during the branching, budding, and flowering stages, respectively, indicating that heat stress to some extent reduces photosynthetic intensity and slows the photosynthetic rate.</p>
<fig id="f5" position="float">
<label>Figure&#xa0;5</label>
<caption>
<p>Trends in gas exchange parameters at different growth stages (<bold>a&#x2013;c</bold> represent the branching, budding, and flowering stages, respectively; <bold>d</bold> shows the overall mean data across the three stages. A denotes photosynthetic rate (A/&#xb5;mol m<sup>-2</sup> s<sup>-1</sup>), gsw represents stomatal conductance (gsw/mol m<sup>-2</sup> s<sup>-1</sup>), and Ci indicates intercellular CO<sub>2</sub> concentration (Ci/&#xb5;mol mol<sup>-1</sup>)).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-17-1745759-g005.tif">
<alt-text content-type="machine-generated">Three bar charts displaying changes in three parameters (A, gsw, Ci) over time, labeled with growth stages (branching, budding, flowering). Each chart compares control (CK) and treatment (T) groups, with error bars indicating variability. Dates and growth stages are shown along the x-axis.</alt-text>
</graphic></fig>
<p>Stomatal conductance (gsw) measurements were consistently lower in T compared to CK across all stages. From branching to flowering, the decrease in stomatal conductance became more pronounced, though the overall trend in both groups was similar&#x2014;initially increasing and then decreasing. In this study, higher stomatal conductance allows more CO<sub>2</sub> to enter cells, resulting in lower intercellular CO<sub>2</sub> concentration (Ci) and higher net photosynthetic rate. When stomata close, Ci also decreases. In contrast to photosynthetic rate and stomatal conductance, T exhibited consistently lower Ci values compared to CK at all measured stages. Across branching, budding, and flowering stages, Ci showed an overall increasing trend, with the average increase growing over time, consistent with the duration of heat stress.</p>
<p>The comparison results of   Fv'/Fm' and qP show that the values in T are consistently lower than those in CK (<xref ref-type="fig" rid="f6"><bold>Figure&#xa0;6</bold></xref>). The overall trend of <inline-formula>
<mml:math display="inline" id="im12"><mml:mrow><mml:mtext>Fv'</mml:mtext><mml:mo stretchy="false">/</mml:mo><mml:mtext>Fm'</mml:mtext></mml:mrow></mml:math></inline-formula> first rises and then declines, with the mean changes across the three stages consistent with multiple measurements, showing decreases of 5.39%, 9.73%, and 9.92% at the branching, budding, and flowering stages, respectively. For qP, T values are also lower than those of CK, with an overall trend from branching to flowering stages consistent with CK, and the mean decrease progressively increasing at 10.83%, 11.37%, and 15.20% respectively. In contrast to <inline-formula>
<mml:math display="inline" id="im13"><mml:mrow><mml:mtext>Fv'</mml:mtext><mml:mo stretchy="false">/</mml:mo><mml:mtext>Fm'</mml:mtext></mml:mrow></mml:math></inline-formula> and qP, the qN values in T were consistently higher than those in CK, increasing by 5.57%, 11.56%, and 5.99% at branching, budding, and flowering stages respectively, showing a trend of first increasing and then decreasing.</p>
<fig id="f6" position="float">
<label>Figure&#xa0;6</label>
<caption>
<p>Trends in fluorescence parameters at different growth stages (<bold>a&#x2013;c</bold> represent the branching, budding, and flowering stages, respectively; <bold>d</bold> shows the overall mean data across the three stages. <inline-formula>
<mml:math display="inline" id="im10"><mml:mrow><mml:mtext>Fv'</mml:mtext><mml:mo stretchy="false">/</mml:mo><mml:mtext>Fm'</mml:mtext></mml:mrow></mml:math></inline-formula> denotes the PSII photochemical efficiency under light, qP represents the photochemical quenching coefficient, and qN indicates the non-photochemical quenching coefficient).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-17-1745759-g006.tif">
<alt-text content-type="machine-generated">Bar chart depicting Fv'/Fm', qP, and qN measurements over dates corresponding to different growth stages: branching, budding, and flowering. Two treatments, CK (white bars) and T (grey bars), are compared. Data shows variation in measurements with error bars indicating variability.</alt-text>
</graphic></fig>
<p>Based on the trends of photosynthetic and fluorescence parameters throughout the entire growth period, the most significant changes among the six photosynthetic parameters are observed in gsw, qP, A, and qN. Changes in gas exchange parameters are more pronounced, with qP and qN showing considerable variation among fluorescence parameters. From these results, sensitive photosynthetic parameters at the branching and flowering stages include gas exchange parameter gsw and fluorescence parameter qP, whereas at the budding stage, sensitive parameters include gas exchange parameter A and fluorescence parameter qN.</p>
</sec>
</sec>
<sec id="s3_2">
<label>3.2</label>
<title>Sensitive spectral bands and features of physiological indicators across growth stages</title>
<sec id="s3_2_1">
<label>3.2.1</label>
<title>Branching stages</title>
<p>The spectral characteristic bands at the branching stage were shown in <xref ref-type="fig" rid="f7"><bold>Figure&#xa0;7</bold></xref>. In the original spectra, the qP characteristic bands in CK were similar to those of gsw, both being concentrated in the near-infrared reflectance plateau. In T, the gsw bands shifted toward longer wavelengths compared with CK, while the qP bands shifted toward shorter wavelengths. In the first-derivative spectra, the sensitive bands of both gsw and qP in T shifted toward longer wavelengths relative to CK.</p>
<fig id="f7" position="float">
<label>Figure&#xa0;7</label>
<caption>
<p>Sensitive bands at different growth stages (<bold>a</bold> original spectra &#x2013; correlation analysis, <bold>b</bold> original spectra &#x2013; SPA, <bold>c</bold> first-derivative spectra &#x2013; correlation analysis, <bold>d</bold> first-derivative spectra &#x2013; SPA).</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-17-1745759-g007.tif">
<alt-text content-type="machine-generated">Scatter plots labeled (a) to (d), showing wavelength in nanometers on the vertical axis against various parameters including SPAD, gsw, qP, A, and qN on the horizontal axis under stages: branching, budding, and flowering. Plots depict data points for CK (blue) and T (orange) across different parameters and stages.</alt-text>
</graphic></fig>
<p>A total of 20 spectral red-edge parameters were selected for analysis, comprising 10 positional parameters, 3 area parameters, and 7 red-edge index parameters. Previous studies have demonstrated that these parameters are highly sensitive to variations in plant growth and physiological status (<xref ref-type="bibr" rid="B16">Guo et&#xa0;al., 2018</xref>; <xref ref-type="bibr" rid="B78">Xie et&#xa0;al., 2018</xref>).</p>
<p>During the branching stage (<xref ref-type="fig" rid="f8"><bold>Figure&#xa0;8a</bold></xref>), the chlorophyll content (SPAD) in CK exhibited the strongest correlation with SD<sub>r</sub>-SD<sub>b</sub> (r = 0.53, p &lt; 0.05), followed by D<sub>r</sub>&#x3001;SD<sub>r</sub>&#x3001;SD<sub>r</sub>/SD<sub>b</sub>&#x3001;SD<sub>y</sub>&#x3001;(SD<sub>r</sub>-SD<sub>b</sub>)/(SD<sub>r</sub>+SD<sub>b</sub>) and D<sub>y</sub>, with correlation coefficients of 0.53, 0.53, 0.51, &#x2212;0.50, 0.47, and &#x2212;0.47, respectively (p &lt; 0.05 for all). In T, the parameter most strongly associated with SPAD was (SD<sub>r</sub>-SD<sub>y</sub>)/(SD<sub>r</sub>+SD<sub>y</sub>) (r = 0.49, p &lt; 0.05), followed by &#x3bb;<sub>v</sub> (r = 0.48) and SD<sub>r</sub>/SD<sub>y</sub> (r = 0.45). Overall, correlations in CK were stronger than those in T.</p>
<fig id="f8" position="float">
<label>Figure&#xa0;8</label>
<caption>
<p>Correlation coefficients between three-edge parameters and physiological indices (<bold>a</bold> branching stage; <bold>b</bold> budding stage; <bold>c</bold> flowering stage). Notes (same below): <italic>D<sub>r</sub></italic> &#x2014; red-edge amplitude; <italic>&#x3bb;<sub>r</sub></italic> &#x2014; red-edge position; <italic>D<sub>b</sub></italic> &#x2014; blue-edge amplitude; <italic>&#x3bb;<sub>b</sub></italic> &#x2014; blue-edge position; <italic>D<sub>y</sub></italic> &#x2014; yellow-edge amplitude; <italic>&#x3bb;<sub>y</sub></italic> &#x2014; yellow-edge position; <italic>R<sub>g</sub></italic> &#x2014; green peak reflectance; <italic>&#x3bb;<sub>g</sub></italic> &#x2014; green peak position; <italic>R<sub>r</sub></italic> &#x2014; red valley amplitude; <italic>&#x3bb;<sub>v</sub></italic> &#x2014; red valley position; <italic>SD<sub>r</sub></italic> &#x2014; red-edge area; <italic>SD<sub>b</sub></italic> &#x2014; blue-edge area; <italic>SD<sub>y</sub></italic> &#x2014; yellow-edge area; (<italic>R<sub>g</sub></italic> &#x2013; <italic>R<sub>r</sub></italic>)/(<italic>R<sub>g</sub></italic> + <italic>R<sub>r</sub></italic>) &#x2014; normalized difference of green peak and red valley reflectance; <italic>R<sub>g</sub></italic>/<italic>R<sub>r</sub></italic> &#x2014; ratio of green peak to red valley reflectance; <italic>SD<sub>r</sub></italic>/<italic>SD<sub>b</sub></italic> &#x2014; ratio of red-edge area to blue-edge area; <italic>SD<sub>r</sub></italic>/<italic>SD<sub>y</sub></italic> &#x2014; ratio of red-edge area to yellow-edge area; <italic>SD<sub>r</sub></italic> &#x2013; <italic>SD<sub>b</sub></italic> &#x2014; difference between red-edge area and blue-edge area; (<italic>SD<sub>r</sub></italic> &#x2013; <italic>SD<sub>b</sub></italic>)/(<italic>SD<sub>r</sub></italic> + <italic>SD<sub>b</sub></italic>) &#x2014; normalized difference of red-edge area and blue-edge area; (<italic>SD<sub>r</sub></italic> &#x2013; <italic>SD<sub>y</sub></italic>)/(<italic>SD<sub>r</sub></italic> + <italic>SD<sub>y</sub></italic>) &#x2014; normalized difference of red-edge area and yellow-edge area.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-17-1745759-g008.tif">
<alt-text content-type="machine-generated">Scatter plots showing correlation coefficients of triangular spectral parameters across three panels: (a), (b), and (c). Various colored and shaped markers indicate different variables such as SPAD_CK, gsw_CK, qP_CK, SPAD_T, gsw_T, and qP_T. The x-axis represents triangular spectral parameters like DrL, Drb, Dyr, and more, while the y-axis shows correlation coefficients from negative one to positive one.</alt-text>
</graphic></fig>
<p>For photosynthetic parameters during the branching stage, gsw in CK showed extremely significant correlations with D<sub>y</sub> (r = 0.69) and R<sub>f</sub> (r = 0.73). qP was also extremely significantly correlated with &#x3bb;<sub>b</sub> (r = &#x2212;0.65), R<sub>g</sub> (r = &#x2212;0.79), (SD<sub>r</sub>-SD<sub>b</sub>)/(SD<sub>r</sub>+SD<sub>b</sub>) (r = &#x2212;0.69), and (SD<sub>r</sub>-SD<sub>y</sub>)/(SD<sub>r</sub>+SD<sub>y</sub>) (r = &#x2212;0.75). In T, gsw responded most strongly to &#x3bb;<sub>r</sub> (r = 0.68), SD<sub>r</sub> (r = 0.64), SD<sub>r</sub>/SD<sub>b</sub> (r = 0.56), and SD<sub>r</sub>-SD<sub>b</sub> (r = 0.65). qP exhibited the highest correlations with R<sub>g</sub> (r = 0.57), R<sub>r</sub> (r = 0.71), R<sub>g</sub>/R<sub>r</sub> (r = 0.68), SD<sub>r</sub>/SD<sub>b</sub> (r = &#x2212;0.88), SD<sub>r</sub>-SD<sub>b</sub> (r = 0.62), and (SD<sub>r</sub>-SD<sub>b</sub>)/(SD<sub>r</sub>+SD<sub>b</sub>) (r = &#x2212;0.77).</p>
<p>Overall, the three indicators (SPAD, gsw, and qP) generally exhibited stronger correlations with red-edge parameters in CK than in T. Among these, photosynthetic parameters displayed stronger associations than SPAD. Within T, qP demonstrated the highest sensitivity to temperature changes, suggesting its potential as a key indicator for assessing heat stress responses.</p>
<p>During the branching stage, the SPAD-sensitive bands were primarily distributed in the infrared region (<xref ref-type="table" rid="T2"><bold>Table&#xa0;2</bold></xref>). In CK, the SPAD values from the original spectra showed the strongest correlation with DVI (553, 705) (r = 0.80), while the SPAD values from the first-derivative spectra were most strongly correlated with FDNDVI (1083, 922) (r = 0.87). In T, the SPAD values from the original spectra exhibited the strongest correlations with NDVI (891, 890) and DVI (891, 890) (both r = 0.50), whereas the SPAD values from the first-derivative spectra were most strongly correlated with FDDVI (849, 844) (r = 0.81).</p>
<table-wrap id="T2" position="float">
<label>Table&#xa0;2</label>
<caption>
<p>Branching stage: optimal vegetation index bands and corresponding correlation coefficients.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" colspan="2" align="center">Physiological indicators</th>
<th valign="middle" colspan="2" align="center">SPAD</th>
<th valign="middle" colspan="2" align="center">gsw</th>
<th valign="middle" colspan="2" align="center">qP</th>
</tr>
<tr>
<th valign="middle" colspan="2" align="center">Group</th>
<th valign="middle" align="center">CK</th>
<th valign="middle" align="center">T</th>
<th valign="middle" align="center">CK</th>
<th valign="middle" align="center">T</th>
<th valign="middle" align="center">CK</th>
<th valign="middle" align="center">T</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" rowspan="2" align="center">RVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">779,777</td>
<td valign="middle" align="center">891,890</td>
<td valign="middle" align="center">691,630</td>
<td valign="middle" align="center">1044,968</td>
<td valign="middle" align="center">827,828</td>
<td valign="middle" align="center">1002,981</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.72</td>
<td valign="middle" align="center">0.49</td>
<td valign="middle" align="center">0.65</td>
<td valign="middle" align="center">0.53</td>
<td valign="middle" align="center">0.49</td>
<td valign="middle" align="center">0.83</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">NDVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">779,777</td>
<td valign="middle" align="center">819,890</td>
<td valign="middle" align="center">691,630</td>
<td valign="middle" align="center">1044,968</td>
<td valign="middle" align="center">827,828</td>
<td valign="middle" align="center">1002,981</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.73</td>
<td valign="middle" align="center">0.5</td>
<td valign="middle" align="center">0.65</td>
<td valign="middle" align="center">0.53</td>
<td valign="middle" align="center">0.49</td>
<td valign="middle" align="center">0.83</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">DVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">553,705</td>
<td valign="middle" align="center">891,890</td>
<td valign="middle" align="center">772,780</td>
<td valign="middle" align="center">1088,958</td>
<td valign="middle" align="center">827,829</td>
<td valign="middle" align="center">997,981</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.8</td>
<td valign="middle" align="center">0.5</td>
<td valign="middle" align="center">0.59</td>
<td valign="middle" align="center">0.53</td>
<td valign="middle" align="center">0.51</td>
<td valign="middle" align="center">0.81</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">FDRVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">800,987</td>
<td valign="middle" align="center">457,1109</td>
<td valign="middle" align="center">991,1275</td>
<td valign="middle" align="center">844,848</td>
<td valign="middle" align="center">939,1273</td>
<td valign="middle" align="center">1264,805</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.84</td>
<td valign="middle" align="center">0.7</td>
<td valign="middle" align="center">0.76</td>
<td valign="middle" align="center">0.73</td>
<td valign="middle" align="center">0.77</td>
<td valign="middle" align="center">0.84</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">FDNDVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">1083,922</td>
<td valign="middle" align="center">1110,1006</td>
<td valign="middle" align="center">937,628</td>
<td valign="middle" align="center">844,849</td>
<td valign="middle" align="center">1247,847</td>
<td valign="middle" align="center">982,1002</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.87</td>
<td valign="middle" align="center">0.78</td>
<td valign="middle" align="center">0.79</td>
<td valign="middle" align="center">0.73</td>
<td valign="middle" align="center">0.76</td>
<td valign="middle" align="center">0.85</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">FDDVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">850,823</td>
<td valign="middle" align="center">849,844</td>
<td valign="middle" align="center">956,966</td>
<td valign="middle" align="center">988,372</td>
<td valign="middle" align="center">891,890</td>
<td valign="middle" align="center">982,918</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.85</td>
<td valign="middle" align="center">0.81</td>
<td valign="middle" align="center">0.68</td>
<td valign="middle" align="center">0.71</td>
<td valign="middle" align="center">0.71</td>
<td valign="middle" align="center">0.9</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>For photosynthetic parameters in the branching stage, the optimal index for gsw in CK was the first derivative spectral index FDNDVI (937, 628) (r = 0.79), while the optimal index for qP was FDRVI (939, 1273) (r = 0.77). In T, the optimal indices for gsw were FDNDVI (844, 849) and FDRVI (844, 848), both with r = 0.73, and the optimal index for qP was FDDVI (982, 918) (r = 0.90). The two photosynthetic parameters exhibited contrasting spectral responses between treatments: gsw showed stronger spectral responsiveness in CK compared to T, whereas qP was more responsive in T than in CK.</p>
</sec>
<sec id="s3_2_2">
<label>3.2.2</label>
<title>Budding stage</title>
<p>In the budding stage, the sensitive wavelengths of A in the original spectrum for T shifted toward shorter wavelengths compared to CK, with qN showing the same shift direction as A; however, in the first derivative spectrum, the sensitive wavelengths of both A and qN for T shifted toward longer wavelengths relative to CK (<xref ref-type="fig" rid="f7"><bold>Figure&#xa0;7</bold></xref>).</p>
<p>During the budding stage (<xref ref-type="fig" rid="f8"><bold>Figure&#xa0;8b</bold></xref>), the spectral feature parameter that was most strongly correlated with chlorophyll content in CK was SDr, with a correlation coefficient of 0.97 (p &lt; 0.01). Other parameters that showed high correlations included (SDr-SDb)/(SDr+SDb), (SDr-SDy)/(SDr+SDy), SDr/SDb, &#x3bb;r, and SDy, with respective correlation coefficients of 0.86, 0.85, 0.80, 0.61, and 0.59, all at a highly significant level. For T during the budding stage, the spectral parameter most correlated with chlorophyll content was SDr-SDb, with a correlation coefficient of 0.63 (p &lt; 0.01). Other parameters that had notable correlations were Dr and &#x3bb;b, with coefficients of 0.56 and -0.54, significant at the 0.05 level.</p>
<p>For CK in the budding stage, A showed highly significant correlations with &#x3bb;<sub>b</sub>, D<sub>y</sub>, and (SD<sub>r</sub>-SD<sub>y</sub>)/(SD<sub>r</sub>+SD<sub>y</sub>), with coefficients of -0.77, 0.66, and -0.67, respectively. qN was highly correlated with D<sub>r</sub>, SD<sub>r</sub>, SD<sub>r</sub>-SD<sub>b</sub>, and (SD<sub>r</sub>-SD<sub>b</sub>)/(SD<sub>r</sub>+SD<sub>b</sub>), with coefficients of 0.87, 0.76, 0.77, and 0.73. In T, A was highly correlated with &#x3bb;<sub>r</sub>, (SD<sub>r</sub>-SD<sub>b</sub>)/(SD<sub>r</sub>+SD<sub>b</sub>), and (SD<sub>r</sub>-SD<sub>y</sub>)/(SD<sub>r</sub>+SD<sub>y</sub>), with coefficients of 0.68, 0.68, and -0.71. qN showed strong correlations with D<sub>r</sub>, (R<sub>g</sub>-R<sub>r</sub>)/(R<sub>g</sub>+R<sub>r</sub>), R<sub>g</sub>/R<sub>r</sub>, and SD<sub>r</sub>-SD<sub>b</sub>, with coefficients of 0.57, 0.79, 0.80, and 0.61.</p>
<p>During the budding stage, the SPAD-sensitive bands in CK were primarily concentrated in the infrared region (<xref ref-type="table" rid="T3"><bold>Table 3</bold></xref>), whereas those in T were more widely dispersed. In CK, the SPAD values derived from the original spectra exhibited strong correlations with RVI (1150,1347) and NDVI (1151,1347), with correlation coefficients of 0.77. The first derivative spectra showed the highest correlation with FDRVI (1161,1156), with a coefficient of 0.82. In T, SPAD values from the original spectra were most strongly correlated with RVI (683,666) and NDVI (683,666) (correlation coefficient = 0.55), while the first derivative spectra were most strongly correlated with FDNDVI (1170,388) (correlation coefficient = 0.82).</p>
<table-wrap id="T3" position="float">
<label>Table&#xa0;3</label>
<caption>
<p>Budding stage: optimal vegetation index bands and correlation coefficients.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" colspan="2" align="center">Physiological indicators</th>
<th valign="middle" colspan="2" align="center">SPAD</th>
<th valign="middle" colspan="2" align="center">A</th>
<th valign="middle" colspan="2" align="center">qN</th>
</tr>
<tr>
<th valign="middle" colspan="2" align="center">Group</th>
<th valign="middle" align="center">CK</th>
<th valign="middle" align="center">T</th>
<th valign="middle" align="center">CK</th>
<th valign="middle" align="center">T</th>
<th valign="middle" align="center">CK</th>
<th valign="middle" align="center">T</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" rowspan="2" align="center">RVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">1150,1347</td>
<td valign="middle" align="center">683,666</td>
<td valign="middle" align="center">990,972</td>
<td valign="middle" align="center">1261,1147</td>
<td valign="middle" align="center">971,987</td>
<td valign="middle" align="center">659,660</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.77</td>
<td valign="middle" align="center">0.55</td>
<td valign="middle" align="center">0.85</td>
<td valign="middle" align="center">0.52</td>
<td valign="middle" align="center">0.86</td>
<td valign="middle" align="center">0.57</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">NDVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">1150,1347</td>
<td valign="middle" align="center">683,666</td>
<td valign="middle" align="center">990,972</td>
<td valign="middle" align="center">1261,1147</td>
<td valign="middle" align="center">971,987</td>
<td valign="middle" align="center">659,660</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.77</td>
<td valign="middle" align="center">0.55</td>
<td valign="middle" align="center">0.85</td>
<td valign="middle" align="center">0.52</td>
<td valign="middle" align="center">0.86</td>
<td valign="middle" align="center">0.57</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">DVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">1158,1172</td>
<td valign="middle" align="center">909,908</td>
<td valign="middle" align="center">991,972</td>
<td valign="middle" align="center">1245,1152</td>
<td valign="middle" align="center">972,987</td>
<td valign="middle" align="center">668,678</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.71</td>
<td valign="middle" align="center">0.45</td>
<td valign="middle" align="center">0.85</td>
<td valign="middle" align="center">0.53</td>
<td valign="middle" align="center">0.86</td>
<td valign="middle" align="center">0.48</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">FDRVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">1161,1156</td>
<td valign="middle" align="center">479,980</td>
<td valign="middle" align="center">980,455</td>
<td valign="middle" align="center">778,1266</td>
<td valign="middle" align="center">927,898</td>
<td valign="middle" align="center">671,892</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.82</td>
<td valign="middle" align="center">0.75</td>
<td valign="middle" align="center">0.8</td>
<td valign="middle" align="center">0.71</td>
<td valign="middle" align="center">0.93</td>
<td valign="middle" align="center">0.73</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">FDNDVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">918,760</td>
<td valign="middle" align="center">1170,388</td>
<td valign="middle" align="center">984,411</td>
<td valign="middle" align="center">947,800</td>
<td valign="middle" align="center">1315,1300</td>
<td valign="middle" align="center">599,822</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.8</td>
<td valign="middle" align="center">0.82</td>
<td valign="middle" align="center">0.82</td>
<td valign="middle" align="center">0.77</td>
<td valign="middle" align="center">0.91</td>
<td valign="middle" align="center">0.76</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">FDDVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">1166,372</td>
<td valign="middle" align="center">462,46</td>
<td valign="middle" align="center">984,1090</td>
<td valign="middle" align="center">889,893</td>
<td valign="middle" align="center">898,660</td>
<td valign="middle" align="center">973,916</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.79</td>
<td valign="middle" align="center">0.76</td>
<td valign="middle" align="center">0.85</td>
<td valign="middle" align="center">0.61</td>
<td valign="middle" align="center">0.89</td>
<td valign="middle" align="center">0.72</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>For the photosynthetic parameter A in CK, all four vegetation indices except FDNDVI and FDRVI showed high correlations (r = 0.85) with optimal bands of NDVI (990,972), DVI (991,972), RVI (990,972), and FDDVI (984,1090). In T, the optimal index was FDNDVI (947,800), with a correlation coefficient of 0.77. For the photosynthetic parameter qN, CK exhibited the highest correlation with FDRVI (927,898) (r = 0.93), while in T the highest correlation was with FDNDVI (599,822) (r = 0.76). Overall, the spectral responses of A and qN during the budding stage were stronger in CK than in T, and vegetation indices derived from first derivative spectra showed better performance than those from the original spectra.</p>
</sec>
<sec id="s3_2_3">
<label>3.2.3</label>
<title>Flowering stage</title>
<p>Based on correlation analysis and the SPA algorithm, the sensitive bands of physiological indices during the flowering stage were identified (<xref ref-type="fig" rid="f7"><bold>Figure&#xa0;7</bold></xref>). For the raw spectra, the sensitive bands of gsw in T shifted toward shorter wavelengths compared with CK, and qP exhibited a similar shift direction to gsw. In the first derivative spectra, the sensitive bands of gsw in T also shifted toward shorter wavelengths relative to CK, whereas qP shifted in the opposite direction, toward longer wavelengths.</p>
<p>During the flowering stage (<xref ref-type="fig" rid="f8"><bold>Figure&#xa0;8c</bold></xref>), the spectral characteristic parameter most strongly correlated with chlorophyll content in CK was (SD<sub>r</sub>&#x2212;SD<sub>b</sub>)/(SD<sub>r</sub> + SD<sub>b</sub>), with a correlation coefficient of 0.62 (p &lt; 0.01). Other parameters significantly correlated at the 0.01 level included &#x3bb;<sub>r</sub>, SD<sub>r</sub>/SD<sub>b</sub>, (SD<sub>r</sub>-SD<sub>y</sub>)/(SD<sub>r</sub>+SD<sub>y</sub>), and SD<sub>r</sub>/SD<sub>y</sub>, with coefficients of 0.60, 0.58, 0.57, and 0.57, respectively. Parameters correlated at the 0.05 level included &#x3bb;<sub>y</sub>, SD<sub>r</sub>-SD<sub>b</sub>,SD<sub>r</sub>, &#x3bb;<sub>b</sub>, and D<sub>r</sub>, with coefficients of 0.53, 0.50, 0.47, 0.46, and 0.46, respectively. In the branching stage, the spectral parameter most strongly correlated with chlorophyll content in T was &#x3bb;<sub>y</sub>, with a correlation coefficient of &#x2212;0.68 (p &lt; 0.01).</p>
<p>During the flowering stage, in CK, gsw showed extremely significant correlations with D<sub>r</sub>, SD<sub>r</sub>-SD<sub>b</sub>, and (SD<sub>r</sub>-SD<sub>b</sub>)/(SD<sub>r</sub>+SD<sub>b</sub>), with correlation coefficients of &#x2212;0.87, &#x2212;0.83, and &#x2212;0.81, respectively. qP was extremely significantly correlated with D<sub>r</sub>, SD<sub>r</sub>, SD<sub>r</sub> &#x2212; SD<sub>b</sub>, and (SD<sub>r</sub> &#x2212; SD<sub>b</sub>)/(SD<sub>r</sub> + SD<sub>b</sub>), with coefficients of 0.87, 0.86, 0.87, and 0.73, respectively. In T, gsw was extremely significantly correlated with D<sub>r</sub>, &#x3bb;<sub>y</sub>, SD<sub>r</sub>, SD<sub>y</sub>, (R<sub>g</sub> &#x2212; R<sub>r</sub>)/(R<sub>g</sub> + R<sub>r</sub>), R<sub>g</sub>/R<sub>r</sub>, and SD<sub>r</sub>-SD<sub>b</sub>, with correlation coefficients of &#x2212;0.72, &#x2212;0.65, &#x2212;0.93, 0.64, &#x2212;0.57, &#x2212;0.58, and &#x2212;0.92, respectively. qP exhibited extremely significant correlations with D<sub>r</sub>, &#x3bb;<sub>y</sub>, SD<sub>r</sub>, R<sub>g</sub>/R<sub>r</sub>, SD<sub>r</sub>/SD<sub>b</sub>, SD<sub>r</sub>-SD<sub>b</sub>, and (SD<sub>r</sub>-SD<sub>b</sub>)/(SD<sub>r</sub>+SD<sub>b</sub>), with coefficients of 0.86, 0.67, 0.58, 0.74, 0.77, 0.87, and 0.71, respectively.</p>
<p>During the flowering stage, the SPAD-sensitive bands were mainly distributed in the infrared region (<xref ref-type="table" rid="T4"><bold>Table 4</bold></xref>). In CK, the SPAD values from the original spectra showed a strong correlation with DVI (920, 919) (r = 0.69), while the SPAD values from the first derivative spectra exhibited the same correlation coefficient (r = 0.80) with FDDVI (862, 861), FDNDVI (862, 861), and FDRVI (913, 919). In T, the SPAD values from the original spectra were most strongly correlated with DVI (977, 975) (r = 0.66), whereas the first derivative spectra showed the highest correlation with FDDVI (862, 861) (r = 0.73).</p>
<table-wrap id="T4" position="float">
<label>Table&#xa0;4</label>
<caption>
<p>Flowering stage: optimal vegetation index bands and correlation coefficients.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" colspan="2" align="center">Physiological indicators</th>
<th valign="middle" colspan="2" align="center">SPAD</th>
<th valign="middle" colspan="2" align="center">gsw</th>
<th valign="middle" colspan="2" align="center">qP</th>
</tr>
<tr>
<th valign="middle" colspan="2" align="center">Group</th>
<th valign="middle" align="center">CK</th>
<th valign="middle" align="center">T</th>
<th valign="middle" align="center">CK</th>
<th valign="middle" align="center">T</th>
<th valign="middle" align="center">CK</th>
<th valign="middle" align="center">T</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" rowspan="2" align="center">RVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">920,919</td>
<td valign="middle" align="center">977,975</td>
<td valign="middle" align="center">1273,1272</td>
<td valign="middle" align="center">695,350</td>
<td valign="middle" align="center">1337,726</td>
<td valign="middle" align="center">1328,723</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.69</td>
<td valign="middle" align="center">0.66</td>
<td valign="middle" align="center">0.74</td>
<td valign="middle" align="center">0.82</td>
<td valign="middle" align="center">0.53</td>
<td valign="middle" align="center">0.62</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">NDVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">920,919</td>
<td valign="middle" align="center">963,962</td>
<td valign="middle" align="center">1273,1272</td>
<td valign="middle" align="center">697,350</td>
<td valign="middle" align="center">1337,726</td>
<td valign="middle" align="center">1327,723</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.68</td>
<td valign="middle" align="center">0.6</td>
<td valign="middle" align="center">0.74</td>
<td valign="middle" align="center">0.83</td>
<td valign="middle" align="center">0.53</td>
<td valign="middle" align="center">0.62</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">DVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">920,919</td>
<td valign="middle" align="center">963,962</td>
<td valign="middle" align="center">916,915</td>
<td valign="middle" align="center">585,584</td>
<td valign="middle" align="center">1320,718</td>
<td valign="middle" align="center">870,868</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.68</td>
<td valign="middle" align="center">0.6</td>
<td valign="middle" align="center">0.72</td>
<td valign="middle" align="center">0.78</td>
<td valign="middle" align="center">0.72</td>
<td valign="middle" align="center">0.59</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">FDRVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">862,861</td>
<td valign="middle" align="center">862,861</td>
<td valign="middle" align="center">922,875</td>
<td valign="middle" align="center">1270,901</td>
<td valign="middle" align="center">594,959</td>
<td valign="middle" align="center">902,891</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.8</td>
<td valign="middle" align="center">0.73</td>
<td valign="middle" align="center">0.87</td>
<td valign="middle" align="center">0.84</td>
<td valign="middle" align="center">0.71</td>
<td valign="middle" align="center">0.74</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">FDNDVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">862,861</td>
<td valign="middle" align="center">862,861</td>
<td valign="middle" align="center">416,934</td>
<td valign="middle" align="center">1001,1004</td>
<td valign="middle" align="center">595,594</td>
<td valign="middle" align="center">505,561</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.8</td>
<td valign="middle" align="center">0.69</td>
<td valign="middle" align="center">0.9</td>
<td valign="middle" align="center">0.84</td>
<td valign="middle" align="center">0.78</td>
<td valign="middle" align="center">0.72</td>
</tr>
<tr>
<td valign="middle" rowspan="2" align="center">FDDVI</td>
<td valign="middle" align="center">Wavelength combination</td>
<td valign="middle" align="center">913,919</td>
<td valign="middle" align="center">913,919</td>
<td valign="middle" align="center">646,640</td>
<td valign="middle" align="center">588,595</td>
<td valign="middle" align="center">657,492</td>
<td valign="middle" align="center">918,932</td>
</tr>
<tr>
<td valign="middle" align="center">Correlation coefficient</td>
<td valign="middle" align="center">0.8</td>
<td valign="middle" align="center">0.69</td>
<td valign="middle" align="center">0.84</td>
<td valign="middle" align="center">0.85</td>
<td valign="middle" align="center">0.78</td>
<td valign="middle" align="center">0.71</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>For the photosynthetic parameter gsw, the spectral response of T was generally superior to that of CK. The highest correlation coefficient for both groups (r = 0.90) was observed in CK for the first derivative spectral index FDNDVI (416, 934), while T achieved its highest correlation (r = 0.85) with FDDVI (588, 595). For the photosynthetic parameter qP, the optimal spectral indices in CK were FDNDVI (595, 594) and FDDVI (657, 492), both with correlation coefficients of 0.78, whereas in T the optimal spectral index was FDRVI (902, 891) with a correlation coefficient of 0.74. Overall, the gsw spectral response in CK was superior to that of qP.</p>
</sec>
</sec>
<sec id="s3_3">
<label>3.3</label>
<title>Model prediction of physiological indicators at different growth stages</title>
<p><xref ref-type="fig" rid="f5"><bold>Figure&#xa0;5</bold></xref> shows that during the branching stage, the overall prediction performance of the three models ranked as SVR &gt; PLSR &gt; RFR, with R<sup>2</sup> values for both training and testing sets ranging between 0.6 and 0.9, and training set values generally higher than those of the testing set. The most frequently selected optimal feature was the first-derivative spectral vegetation index FDNDVI, followed by TP and NDVI. Among the three physiological indicators (SPAD, gsw, and qP), the SVR model achieved the best prediction for gsw; the RFR model performed best for qP; and the PLSR model yielded the highest accuracy for SPAD. Overall, the prediction results for alfalfa under normal growth and heat stress conditions showed no significant differences, indicating that early-stage heat stress has limited impact and physiological traits during the branching stage are insufficient to serve as distinguishing markers.</p>
<p>For the budding stage, the prediction performance of the untreated group was better than that of the treated group across the three models. In the SVR model, R&#xb2; values exceeded 0.9 in some cases, with prediction accuracy ranking as SVR &gt; PLSR &gt; RFR. The most frequently selected optimal feature was FDNDVI, followed by NDVI and FDS2. Within the SVR model, the best predicted physiological indicator was A, with NDVI as the optimal feature; for the RFR model, SPAD showed the best prediction, with TP as the optimal feature; and for the PLSR model, qN was best predicted, with FDNDVI as the optimal feature. No clear pattern was observed between CK and T in prediction performance, and RMSE values were generally high.</p>
<p>The model prediction results for the flowering stage showed R&#xb2; values ranging from 0.6 to 1. Overall, the prediction performance ranked as SVR &gt; RFR &gt; PLSR. The most frequently occurring optimal feature remained FDNDVI, followed by NDVI. Within the SVR model, the best predicted physiological indicator was qP, with MDVI as the optimal feature. For the RFR model, gsw had the best prediction performance, with FDNDVI as the optimal feature. In the PLSR model, gsw also showed the best prediction, with NDVI as the optimal feature.</p>
<p>Based on a comprehensive analysis of <xref ref-type="table" rid="T5"><bold>Tables&#xa0;5</bold></xref>&#x2013;<xref ref-type="table" rid="T7"><bold>7</bold></xref>, from the perspective of growth stages, prediction performance evaluated by R&#xb2; indicates that the budding stage outperforms both the flowering and branching stages. The branching stage represents the initial phase of heat stress, during which the impact on alfalfa growth is not significant. However, as heat stress duration increases, its effects become more pronounced. Regarding prediction models, across different growth stages and physiological indicators, all three models show that SVR consistently outperforms RFR and PLSR. The RFR model provides the best prediction for SPAD, while the SVR model yields the best predictions for photosynthetic parameters. Among the best prediction results from branching to flowering stages, the most frequently appearing index is FDNDVI, followed by NDVI, indicating that spectral vegetation indices are the optimal predictive variables.</p>
<table-wrap id="T5" position="float">
<label>Table&#xa0;5</label>
<caption>
<p>Branching stage: optimal spectral features of physiological indicator.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" rowspan="3" align="center">Model</th>
<th valign="middle" rowspan="3" align="center">Physiological indicator</th>
<th valign="middle" rowspan="2" align="center">Treatment</th>
<th valign="middle" colspan="4" align="center">CK</th>
<th valign="middle" rowspan="2" align="center">Treatment</th>
<th valign="middle" colspan="4" align="center">T</th>
</tr>
<tr>
<th valign="middle" colspan="2" align="center">Training set</th>
<th valign="middle" colspan="2" align="center">Testing set</th>
<th valign="middle" colspan="2" align="center">Training set</th>
<th valign="middle" colspan="2" align="center">Testing set</th>
</tr>
<tr>
<th valign="middle" align="center">Feature</th>
<th valign="middle" align="center">R<sub>c1</sub><sup>2</sup></th>
<th valign="middle" align="center">RMSE<sub>c1</sub></th>
<th valign="middle" align="center">R<sub>c2</sub><sup>2</sup></th>
<th valign="middle" align="center">RMSE<sub>c2</sub></th>
<th valign="middle" align="center">Feature</th>
<th valign="middle" align="center">R<sub>t1</sub><sup>2</sup></th>
<th valign="middle" align="center">RMSE<sub>t1</sub></th>
<th valign="middle" align="center">R<sub>t2</sub><sup>2</sup></th>
<th valign="middle" align="center">RMSE<sub>t2</sub></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" rowspan="3" align="center">SVR</td>
<td valign="middle" align="center">SPAD</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.83</td>
<td valign="middle" align="center">3.06</td>
<td valign="middle" align="center">0.79</td>
<td valign="middle" align="center">4.08</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.76</td>
<td valign="middle" align="center">3.55</td>
<td valign="middle" align="center">0.74</td>
<td valign="middle" align="center">2.33</td>
</tr>
<tr>
<td valign="middle" align="center">gsw</td>
<td valign="middle" align="center">NDVI</td>
<td valign="middle" align="center">0.84</td>
<td valign="middle" align="center">0.02</td>
<td valign="middle" align="center">0.76</td>
<td valign="middle" align="center">0.03</td>
<td valign="middle" align="center">NDVI</td>
<td valign="middle" align="center">0.88</td>
<td valign="middle" align="center">0.01</td>
<td valign="middle" align="center">0.76</td>
<td valign="middle" align="center">0.03</td>
</tr>
<tr>
<td valign="middle" align="center">qP</td>
<td valign="middle" align="center">FDS2</td>
<td valign="middle" align="center">0.84</td>
<td valign="middle" align="center">0.04</td>
<td valign="middle" align="center">0.73</td>
<td valign="middle" align="center">0.05</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.84</td>
<td valign="middle" align="center">0.04</td>
<td valign="middle" align="center">0.79</td>
<td valign="middle" align="center">0.05</td>
</tr>
<tr>
<td valign="middle" rowspan="3" align="center">RFR</td>
<td valign="middle" align="center">SPAD</td>
<td valign="middle" align="center">FDS2</td>
<td valign="middle" align="center">0.74</td>
<td valign="middle" align="center">2.73</td>
<td valign="middle" align="center">0.68</td>
<td valign="middle" align="center">4.25</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.69</td>
<td valign="middle" align="center">3.27</td>
<td valign="middle" align="center">0.66</td>
<td valign="middle" align="center">3.73</td>
</tr>
<tr>
<td valign="middle" align="center">gsw</td>
<td valign="middle" align="center">FDS2</td>
<td valign="middle" align="center">0.68</td>
<td valign="middle" align="center">0.03</td>
<td valign="middle" align="center">0.74</td>
<td valign="middle" align="center">0.03</td>
<td valign="middle" align="center">TP</td>
<td valign="middle" align="center">0.74</td>
<td valign="middle" align="center">0.02</td>
<td valign="middle" align="center">0.69</td>
<td valign="middle" align="center">0.02</td>
</tr>
<tr>
<td valign="middle" align="center">qP</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.78</td>
<td valign="middle" align="center">0.04</td>
<td valign="middle" align="center">0.69</td>
<td valign="middle" align="center">0.05</td>
<td valign="middle" align="center">TP</td>
<td valign="middle" align="center">0.81</td>
<td valign="middle" align="center">0.05</td>
<td valign="middle" align="center">0.74</td>
<td valign="middle" align="center">0.05</td>
</tr>
<tr>
<td valign="middle" rowspan="3" align="center">PLSR</td>
<td valign="middle" align="center">SPAD</td>
<td valign="middle" align="center">TP</td>
<td valign="middle" align="center">0.70</td>
<td valign="middle" align="center">2.47</td>
<td valign="middle" align="center">0.60</td>
<td valign="middle" align="center">2.98</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.85</td>
<td valign="middle" align="center">3.14</td>
<td valign="middle" align="center">0.75</td>
<td valign="middle" align="center">3.93</td>
</tr>
<tr>
<td valign="middle" align="center">gsw</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.75</td>
<td valign="middle" align="center">0.04</td>
<td valign="middle" align="center">0.66</td>
<td valign="middle" align="center">0.05</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.73</td>
<td valign="middle" align="center">0.04</td>
<td valign="middle" align="center">0.63</td>
<td valign="middle" align="center">0.05</td>
</tr>
<tr>
<td valign="middle" align="center">qP</td>
<td valign="middle" align="center">OS2</td>
<td valign="middle" align="center">0.71</td>
<td valign="middle" align="center">0.05</td>
<td valign="middle" align="center">0.64</td>
<td valign="middle" align="center">0.06</td>
<td valign="middle" align="center">TP</td>
<td valign="middle" align="center">0.72</td>
<td valign="middle" align="center">0.05</td>
<td valign="middle" align="center">0.65</td>
<td valign="middle" align="center">0.06</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="T6" position="float">
<label>Table&#xa0;6</label>
<caption>
<p>Budding stage: optimal spectral features of physiological indicator.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" rowspan="3" align="center">Model</th>
<th valign="middle" rowspan="3" align="center">Physiological indicator</th>
<th valign="middle" rowspan="2" align="center">Treatment</th>
<th valign="middle" colspan="4" align="center">CK</th>
<th valign="middle" rowspan="2" align="center">Treatment</th>
<th valign="middle" colspan="4" align="center">T</th>
</tr>
<tr>
<th valign="middle" colspan="2" align="center">Training set</th>
<th valign="middle" colspan="2" align="center">Testing set</th>
<th valign="middle" colspan="2" align="center">Training set</th>
<th valign="middle" colspan="2" align="center">Testing set</th>
</tr>
<tr>
<th valign="middle" align="center">Feature</th>
<th valign="middle" align="center">R<sub>c1</sub><sup>2</sup></th>
<th valign="middle" align="center">RMSEc<sub>1</sub></th>
<th valign="middle" align="center">R<sub>c2</sub><sup>2</sup></th>
<th valign="middle" align="center">RMSE<sub>c2</sub></th>
<th valign="middle" align="center">Feature</th>
<th valign="middle" align="center">R<sub>t1</sub><sup>2</sup></th>
<th valign="middle" align="center">RMSE<sub>t1</sub></th>
<th valign="middle" align="center">R<sub>t2</sub><sup>2</sup></th>
<th valign="middle" align="center">RMSE<sub>t2</sub></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" rowspan="3" align="center">SVR</td>
<td valign="middle" align="center">SPAD</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.90</td>
<td valign="middle" align="center">1.45</td>
<td valign="middle" align="center">0.77</td>
<td valign="middle" align="center">1.93</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.86</td>
<td valign="middle" align="center">3.04</td>
<td valign="middle" align="center">0.77</td>
<td valign="middle" align="center">3.50</td>
</tr>
<tr>
<td valign="middle" align="center">A</td>
<td valign="middle" align="center">NDVI</td>
<td valign="middle" align="center">0.91</td>
<td valign="middle" align="center">1.56</td>
<td valign="middle" align="center">0.85</td>
<td valign="middle" align="center">1.67</td>
<td valign="middle" align="center">NDVI</td>
<td valign="middle" align="center">0.96</td>
<td valign="middle" align="center">0.60</td>
<td valign="middle" align="center">0.88</td>
<td valign="middle" align="center">1.39</td>
</tr>
<tr>
<td valign="middle" align="center">qN</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.94</td>
<td valign="middle" align="center">0.03</td>
<td valign="middle" align="center">0.81</td>
<td valign="middle" align="center">0.06</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.95</td>
<td valign="middle" align="center">0.03</td>
<td valign="middle" align="center">0.68</td>
<td valign="middle" align="center">0.07</td>
</tr>
<tr>
<td valign="middle" rowspan="3" align="center">RFR</td>
<td valign="middle" align="center">SPAD</td>
<td valign="middle" align="center">FDS1</td>
<td valign="middle" align="center">0.76</td>
<td valign="middle" align="center">2.90</td>
<td valign="middle" align="center">0.68</td>
<td valign="middle" align="center">4.25</td>
<td valign="middle" align="center">TP</td>
<td valign="middle" align="center">0.83</td>
<td valign="middle" align="center">2.25</td>
<td valign="middle" align="center">0.70</td>
<td valign="middle" align="center">2.38</td>
</tr>
<tr>
<td valign="middle" align="center">A</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.80</td>
<td valign="middle" align="center">1.39</td>
<td valign="middle" align="center">0.76</td>
<td valign="middle" align="center">2.23</td>
<td valign="middle" align="center">FDS2</td>
<td valign="middle" align="center">0.71</td>
<td valign="middle" align="center">2.46</td>
<td valign="middle" align="center">0.63</td>
<td valign="middle" align="center">2.03</td>
</tr>
<tr>
<td valign="middle" align="center">qN</td>
<td valign="middle" align="center">FDS2</td>
<td valign="middle" align="center">0.81</td>
<td valign="middle" align="center">0.09</td>
<td valign="middle" align="center">0.70</td>
<td valign="middle" align="center">0.1</td>
<td valign="middle" align="center">NDVI</td>
<td valign="middle" align="center">0.79</td>
<td valign="middle" align="center">0.07</td>
<td valign="middle" align="center">0.65</td>
<td valign="middle" align="center">0.08</td>
</tr>
<tr>
<td valign="middle" rowspan="3" align="center">PLSR</td>
<td valign="middle" align="center">SPAD</td>
<td valign="middle" align="center">FDS1</td>
<td valign="middle" align="center">0.70</td>
<td valign="middle" align="center">2.84</td>
<td valign="middle" align="center">0.93</td>
<td valign="middle" align="center">1.32</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.85</td>
<td valign="middle" align="center">2.76</td>
<td valign="middle" align="center">0.73</td>
<td valign="middle" align="center">3.92</td>
</tr>
<tr>
<td valign="middle" align="center">A</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.83</td>
<td valign="middle" align="center">1.01</td>
<td valign="middle" align="center">0.66</td>
<td valign="middle" align="center">2.00</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.76</td>
<td valign="middle" align="center">1.47</td>
<td valign="middle" align="center">0.65</td>
<td valign="middle" align="center">2.13</td>
</tr>
<tr>
<td valign="middle" align="center">qN</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.87</td>
<td valign="middle" align="center">0.01</td>
<td valign="middle" align="center">0.76</td>
<td valign="middle" align="center">0.06</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.89</td>
<td valign="middle" align="center">0.01</td>
<td valign="middle" align="center">0.72</td>
<td valign="middle" align="center">0.07</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="T7" position="float">
<label>Table&#xa0;7</label>
<caption>
<p>Flowering stage: optimal spectral features of physiological indicator.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" rowspan="3" align="center">Model</th>
<th valign="middle" rowspan="3" align="center">Physiological indicator</th>
<th valign="middle" rowspan="2" align="center">Treatment</th>
<th valign="middle" colspan="4" align="center">CK</th>
<th valign="middle" rowspan="2" align="center">Treatment</th>
<th valign="middle" colspan="4" align="center">T</th>
</tr>
<tr>
<th valign="middle" colspan="2" align="center">Training set</th>
<th valign="middle" colspan="2" align="center">Testing set</th>
<th valign="middle" colspan="2" align="center">Training set</th>
<th valign="middle" colspan="2" align="center">Testing set</th>
</tr>
<tr>
<th valign="middle" align="center">Feature</th>
<th valign="middle" align="center">R<sub>c1</sub><sup>2</sup></th>
<th valign="middle" align="center">RMSEc<sub>1</sub></th>
<th valign="middle" align="center">R<sub>c2</sub><sup>2</sup></th>
<th valign="middle" align="center">RMSE<sub>c2</sub></th>
<th valign="middle" align="center">Feature</th>
<th valign="middle" align="center">R<sub>t1</sub><sup>2</sup></th>
<th valign="middle" align="center">RMSE<sub>t1</sub></th>
<th valign="middle" align="center">R<sub>t2</sub><sup>2</sup></th>
<th valign="middle" align="center">RMSE<sub>t2</sub></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" rowspan="3" align="center">SVR</td>
<td valign="middle" align="center">SPAD</td>
<td valign="middle" align="center">TP</td>
<td valign="middle" align="center">0.76</td>
<td valign="middle" align="center">2.98</td>
<td valign="middle" align="center">0.76</td>
<td valign="middle" align="center">2.55</td>
<td valign="middle" align="center">NDVI</td>
<td valign="middle" align="center">0.71</td>
<td valign="middle" align="center">2.94</td>
<td valign="middle" align="center">0.68</td>
<td valign="middle" align="center">2.83</td>
</tr>
<tr>
<td valign="middle" align="center">gsw</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.89</td>
<td valign="middle" align="center">0.01</td>
<td valign="middle" align="center">0.86</td>
<td valign="middle" align="center">0.02</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.88</td>
<td valign="middle" align="center">0.01</td>
<td valign="middle" align="center">0.79</td>
<td valign="middle" align="center">0.02</td>
</tr>
<tr>
<td valign="middle" align="center">qP</td>
<td valign="middle" align="center">TP</td>
<td valign="middle" align="center">0.88</td>
<td valign="middle" align="center">0.04</td>
<td valign="middle" align="center">0.75</td>
<td valign="middle" align="center">0.06</td>
<td valign="middle" align="center">NDVI</td>
<td valign="middle" align="center">0.96</td>
<td valign="middle" align="center">0.02</td>
<td valign="middle" align="center">0.87</td>
<td valign="middle" align="center">0.04</td>
</tr>
<tr>
<td valign="middle" rowspan="3" align="center">RFR</td>
<td valign="middle" align="center">SPAD</td>
<td valign="middle" align="center">NDVI</td>
<td valign="middle" align="center">0.70</td>
<td valign="middle" align="center">3.21</td>
<td valign="middle" align="center">0.69</td>
<td valign="middle" align="center">2.92</td>
<td valign="middle" align="center">NDVI</td>
<td valign="middle" align="center">0.69</td>
<td valign="middle" align="center">3.06</td>
<td valign="middle" align="center">0.68</td>
<td valign="middle" align="center">3.05</td>
</tr>
<tr>
<td valign="middle" align="center">gsw</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.79</td>
<td valign="middle" align="center">0.01</td>
<td valign="middle" align="center">0.73</td>
<td valign="middle" align="center">0.02</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.83</td>
<td valign="middle" align="center">0.01</td>
<td valign="middle" align="center">0.71</td>
<td valign="middle" align="center">0.01</td>
</tr>
<tr>
<td valign="middle" align="center">qP</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.68</td>
<td valign="middle" align="center">0.06</td>
<td valign="middle" align="center">0.62</td>
<td valign="middle" align="center">0.07</td>
<td valign="middle" align="center">NDVI</td>
<td valign="middle" align="center">0.77</td>
<td valign="middle" align="center">0.06</td>
<td valign="middle" align="center">0.68</td>
<td valign="middle" align="center">0.06</td>
</tr>
<tr>
<td valign="middle" rowspan="3" align="center">PLSR</td>
<td valign="middle" align="center">SPAD</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.74</td>
<td valign="middle" align="center">2.76</td>
<td valign="middle" align="center">0.64</td>
<td valign="middle" align="center">1.49</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.68</td>
<td valign="middle" align="center">3.31</td>
<td valign="middle" align="center">0.63</td>
<td valign="middle" align="center">3.33</td>
</tr>
<tr>
<td valign="middle" align="center">gsw</td>
<td valign="middle" align="center">OS2</td>
<td valign="middle" align="center">0.77</td>
<td valign="middle" align="center">0.02</td>
<td valign="middle" align="center">0.66</td>
<td valign="middle" align="center">0.02</td>
<td valign="middle" align="center">NDVI</td>
<td valign="middle" align="center">0.84</td>
<td valign="middle" align="center">0.01</td>
<td valign="middle" align="center">0.72</td>
<td valign="middle" align="center">0.01</td>
</tr>
<tr>
<td valign="middle" align="center">qP</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.79</td>
<td valign="middle" align="center">0.05</td>
<td valign="middle" align="center">0.66</td>
<td valign="middle" align="center">0.06</td>
<td valign="middle" align="center">FDNDVI</td>
<td valign="middle" align="center">0.66</td>
<td valign="middle" align="center">0.02</td>
<td valign="middle" align="center">0.59</td>
<td valign="middle" align="center">0.06</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</sec>
<sec id="s4" sec-type="discussion">
<label>4</label>
<title>Discussion</title>
<sec id="s4_1">
<label>4.1</label>
<title>Effects of heat stress on alfalfa growth</title>
<p>Vegetation physiological traits and spectral characteristics undergo changes under abiotic stress (<xref ref-type="bibr" rid="B67">Wahid et&#xa0;al., 2007</xref>). Numerous studies have demonstrated that variations in these traits and spectral features caused by stress can serve as important indicators to assess the extent of abiotic stress on vegetation, as well as to evaluate the stress levels experienced by plants. This study focused on alfalfa, a typical herbaceous species used for reclamation on coal gangue dumps, conducting controlled indoor heat stress experiments. Physiological parameters and hyperspectral characteristics of alfalfa at different growth stages under natural conditions and high-temperature treatments were measured to investigate the response of alfalfa to heat stress. Sensitive spectral features were selected to establish physiological parameter models for validation.</p>
<p>Photosynthesis is the fundamental source of energy and material basis for plant growth (<xref ref-type="bibr" rid="B62">Sun et&#xa0;al., 2023</xref>), and as one of the most vital biological processes in plants, it serves as a key indicator of vegetation response to environmental changes (<xref ref-type="bibr" rid="B80">Xu, 2016</xref>). Research indicates that heat stress adversely affects plant photosynthesis; however, non-extreme high temperatures may induce acquired thermotolerance in plants (<xref ref-type="bibr" rid="B54">Shi et&#xa0;al., 2023</xref>). Photosynthetic rate, stomatal conductance, and intercellular CO<sub>2</sub> concentration interact closely, with stomatal conductance affecting the efficiency of CO<sub>2</sub> uptake from the atmosphere, and intercellular CO<sub>2</sub> concentration being a primary factor influencing photosynthetic rate variations (<xref ref-type="bibr" rid="B8">Chen et&#xa0;al., 2010</xref>; <xref ref-type="bibr" rid="B87">Zhang et&#xa0;al., 2023</xref>). Stomata are critical channels for plant life activities, dynamically regulating physiological balance in response to vegetation status changes (<xref ref-type="bibr" rid="B53">Shi and Leng, 1995</xref>; <xref ref-type="bibr" rid="B68">Wang, 2018</xref>). Although stomatal conductance tends to increase with rising temperatures, high heat can inhibit it (<xref ref-type="bibr" rid="B14">Gao et&#xa0;al., 2016</xref>). In this study (<xref ref-type="fig" rid="f5"><bold>Figure&#xa0;5</bold></xref>), stomatal conductance in T was consistently lower than CK, showing a trend of initial increase followed by decrease. Reduced stomatal conductance led to lower intercellular CO<sub>2</sub> concentration in T compared to CK, while photosynthetic rate initially increased but declined over time. The decline in photosynthetic capacity corresponded with a reduction in leaf chlorophyll content, resulting in delayed or slowed vegetation growth (<xref ref-type="bibr" rid="B67">Wahid et&#xa0;al., 2007</xref>), consistent with previous findings (<xref ref-type="bibr" rid="B37">Mu et&#xa0;al., 2014</xref>; <xref ref-type="bibr" rid="B85">Zhang et&#xa0;al., 2024</xref>). Chlorophyll fluorescence, an important indicator of photosynthesis, can be modulated under heat stress to mitigate photodamage (<xref ref-type="bibr" rid="B19">Guo et&#xa0;al., 2006</xref>; <xref ref-type="bibr" rid="B77">Xia et&#xa0;al., 2025</xref>). <xref ref-type="bibr" rid="B73">Wang et&#xa0;al. (2022)</xref> observed in a gradient temperature study that at 120&#xa0;&#xb0;C, <inline-formula>
<mml:math display="inline" id="im14"><mml:mrow><mml:mtext>Fv'</mml:mtext><mml:mo stretchy="false">/</mml:mo><mml:mtext>Fm'</mml:mtext></mml:mrow></mml:math></inline-formula> initially increased then decreased, while qP steadily declined, consistent with results in the present study (<xref ref-type="bibr" rid="B73">Wang et&#xa0;al., 2022</xref>).</p>
<p>The temporal variation trends of raw spectral reflectance were generally similar between T and CK, with T consistently exhibiting higher reflectance. Differences in the visible light range were limited to the budding stage, whereas significant differences in the near-infrared plateau persisted throughout, indicating that alfalfa&#x2019;s near-infrared spectral reflectance is more sensitive to heat stress. Derivative transformations of raw spectra effectively refine spectral feature information (<xref ref-type="bibr" rid="B95">Zornoza et&#xa0;al., 2008</xref>). By constructing vegetation indices and triangular spectral parameters, combined with correlation analysis and the Successive Projections Algorithm (SPA), sensitive spectral features were identified alongside SPAD and photosynthetic parameter data. The study found that sensitive spectral bands for physiological indicators at different growth stages were mainly distributed in the infrared region, with first-derivative spectral vegetation indices showing stronger correlations, consistent with previous research (<xref ref-type="bibr" rid="B18">Guo et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B21">He et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B35">Luo et&#xa0;al., 2022</xref>). Regression analysis methods yielded satisfactory predictive performance (<xref ref-type="bibr" rid="B34">Liu et&#xa0;al., 2017</xref>). Among the three regression models&#x2014;Support Vector Regression (SVR), Partial Least Squares Regression (PLSR), and Random Forest Regression (RFR)&#x2014;SVR consistently achieved the best prediction accuracy across the three growth stages. The budding stage exhibited the highest predictive precision, with T&#x2019;s SPAD predicted using FDNDVI (R&#xb2; = 0.77, RMSE&#xa0;=&#xa0;3.50). The spectral response correlation of photosynthetic parameters across growth stages aligned with SPAD results, with vegetation indices again providing the best model predictions; NDVI yielded optimal results (A: R&#xb2; = 0.88, RMSE&#xa0;=&#xa0;1.39; qN: R&#xb2; = 0.68, RMSE&#xa0;=&#xa0;0.07). The high accuracy of vegetation physiological parameter prediction models constructed using vegetation indices demonstrates the potential of spectral data in studying vegetation responses to heat stress. This approach can play an indispensable role in monitoring and early warning of spontaneous combustion risks on coal gangue dumps. Future integration with remote sensing imagery could enable assessment of vegetation heat stress intensity, identification of early potential combustion points, reduction of fieldwork, and minimization of reclamation losses in coal mining areas.</p>
</sec>
<sec id="s4_2">
<label>4.2</label>
<title>Mechanisms of heat stress effects on alfalfa physiological parameters and spectral responses</title>
<p>Spontaneous combustion of coal gangue dumps leads to increased soil temperature and alterations in soil physicochemical properties. Previous studies have shown that elevated soil temperature is a dominant factor affecting vegetation growth on coal gangue dumps (<xref ref-type="bibr" rid="B42">Ren et&#xa0;al., 2023</xref>). Soil temperature directly impacts plant roots, thereby influencing the transport of internal hormones within vegetation (<xref ref-type="bibr" rid="B62">Sun et&#xa0;al., 2023</xref>). Heat stress in the root zone had a stronger effect on vegetation compared with aerial heat stress, leading to more pronounced plant damage (<xref ref-type="bibr" rid="B40">Pramanik et&#xa0;al., 2018</xref>). Heat stress negatively affects vegetation growth (<xref ref-type="bibr" rid="B67">Wahid et&#xa0;al., 2007</xref>), with the severity depending on both the intensity and duration of the heat stress (<xref ref-type="bibr" rid="B24">H&#xfc;ve et&#xa0;al., 2011</xref>), as well as the specific growth stage of the plants. High temperatures can inhibit seedling emergence, cause leaf wilting and senescence (<xref ref-type="bibr" rid="B4">Bahuguna and Jagadish, 2015</xref>), and may inflict irreversible damage to the photosynthetic apparatus (<xref ref-type="bibr" rid="B36">Mathur et&#xa0;al., 2014</xref>). Anatomically and morphologically, heat stress results in smaller plant cells, enhanced transpiration, water loss leading to stomatal closure, and reduced stomatal conductance (<xref ref-type="bibr" rid="B14">Gao et&#xa0;al., 2016</xref>), along with thickening of root xylem vessels (<xref ref-type="bibr" rid="B5">Ba&#xf1;on et&#xa0;al., 2004</xref>; <xref ref-type="bibr" rid="B94">Zhu et&#xa0;al., 2011</xref>). Plant functional morphology reflects the physiological state of vegetation, while physiological parameters serve as indicators of plant vitality (<xref ref-type="bibr" rid="B47">Ricotta et&#xa0;al., 2015</xref>). Vegetation spectral curves exhibit distinct &#x201c;peaks&#x201d; and &#x201c;valleys,&#x201d; with leaf reflectance at various wavelengths closely linked to cellular structure and physiological traits. Consequently, correlations between physiological parameters and spectral responses exist, enabling the widespread application of hyperspectral remote sensing technology in plant research (<xref ref-type="bibr" rid="B12">Elvidge, 1990</xref>; <xref ref-type="bibr" rid="B28">Kokaly et&#xa0;al., 2009</xref>; <xref ref-type="bibr" rid="B66">Violle et&#xa0;al., 2007</xref>).Under heat stress, photosynthesis weakens and intercellular CO<sub>2</sub> concentration decreases. Heat stress significantly alters leaf reflectance spectral characteristics, with the shortwave red-edge region (680&#x2013;750 nm) exhibiting &#x201c;red-shift&#x201d; or &#x201c;blue-shift&#x201d; phenomena, directly reflecting heat effects on the spectrum. In the experiment, heat stress also induced a reduction in leaf water content, which was manifested by an increase in reflectance within the shortwave infrared (SWIR) region, indicating that temperature exerted a regulatory effect on the leaf water status. Differences in correlation coefficients between various vegetation indices and spectral bands suggest that heat stress can be identified and quantified using specific spectral indices. The use of sensitive bands enhanced by first-derivative spectra or distinct triangular spectral parameters facilitates improved sensitivity in monitoring subtle physiological changes.</p>
</sec>
<sec id="s4_3">
<label>4.3</label>
<title>Limitations and future perspectives</title>
<p>This study investigated the spectral response patterns of physiological indicators in alfalfa under heat stress by measuring photosynthetic parameters and canopy spectral data. It aimed to clarify the optimal monitoring period and data processing models for alfalfa as the observation target. However, several limitations remain. The best observation period identified was the budding stage. Hyperspectral data were collected using a spectrometer, and morphological differences across alfalfa&#x2019;s growth stages may have introduced variability in data accuracy. Additionally, the predictive models employed were empirical and not specifically optimized, which may have affected the precision of results. Improving accuracy will require validation with larger datasets. Moreover, spontaneous combustion of coal gangue dumps is a dynamic process, whereas this study utilized a constant temperature experiment, thus differing from the actual field conditions.</p>
<p>In summary, heat stress influences vegetation physiological activities and spectral characteristics. The coupling mechanism between physiological and spectral responses induced by heat stress not only deepens understanding of plant stress physiology but also provides theoretical support for remote sensing&#x2013;based heat stress monitoring. Future research should focus on dynamic vegetation observation under variable temperature conditions to explore alfalfa&#x2019;s spectral response characteristics and differences in heat stress responses. This will enhance the adaptability and accuracy of hyperspectral technology for monitoring spontaneous combustion in coal gangue dumps, offering valuable support for early warning systems.</p>
</sec>
</sec>
<sec id="s5" sec-type="conclusions">
<label>5</label>
<title>Conclusions</title>
<p>This study used alfalfa as the research object. By conducting simulated high-temperature stress experiments representative of coal gangue dumps, SPAD, six photosynthetic parameters, and corresponding time-series spectral characteristics were obtained. Prediction models linking physiological indicators with spectral parameters were established to explore the response relationships between plant physiological traits and spectral features. The main conclusions are summarized as follows:</p>
<list list-type="order">
<list-item>
<p>The SPAD values and photosynthetic parameters of alfalfa in both the CK and T groups showed similar temporal patterns across growth stages, characterized by an initial increase followed by a decline. However, heat stress significantly reduced the levels and variation amplitudes of these indicators in the T group. Among the photosynthetic parameters, gsw and qP responded most strongly during the branching and flowering stages, whereas A and qN were more sensitive during the budding stage.</p></list-item>
<list-item>
<p>Correlation analysis between physiological indicators and spectral features, including raw spectra, first-derivative spectra, and triangular parameters, indicated that FDNDVI and FDDVI exhibited the strongest responses under different treatments. First-derivative spectral features showed higher correlations with SPAD than raw spectra, while index-based spectral features were more strongly correlated with photosynthetic parameters.</p></list-item>
<list-item>
<p>Among the three predictive models (SVR, RFR, and PLSR), the SVR model achieved the best performance for both SPAD and photosynthetic parameter prediction, with optimal results obtained during the budding stage under the T group. Overall, FDNDVI and NDVI consistently yielded higher predictive accuracy, suggesting that spectral vegetation indices have the greatest potential for heat stress diagnosis during the budding stage.</p></list-item>
</list>
<p>Coal gangue spontaneous combustion is a dynamic process accompanied by temporal variations in soil temperature. As this study only considered constant-temperature scenarios, future research should integrate dynamic temperature simulations with field observations to improve the applicability and reliability of predictive models for coal gangue spontaneous combustion monitoring and early warning.</p>
</sec>
</body>
<back>
<sec id="s6" sec-type="data-availability">
<title>Data availability statement</title>
<p>The raw data supporting the conclusions of this article will be made available by the authors, without undue reservation.</p></sec>
<sec id="s7" sec-type="author-contributions">
<title>Author contributions</title>
<p>MH: Data curation, Formal Analysis, Methodology, Software, Validation, Visualization, Writing &#x2013; original draft. HR: Funding acquisition, Supervision, Writing &#x2013; review &amp; editing. YZ:&#xa0;Conceptualization, Funding acquisition, Resources, Writing &#x2013; review &amp; editing. TH: Supervision, Writing &#x2013; review &amp; editing. CC: Conceptualization, Data curation, Formal Analysis, Investigation, Software, Validation, Writing &#x2013; review &amp; editing. LZ: Writing &#x2013; review &amp; editing. YT: Writing &#x2013; review &amp; editing.</p></sec>
<ack>
<title>Acknowledgments</title>
<p>We are immensely grateful to the editor and reviewers for their comments on the manuscript.</p>
</ack>
<sec id="s9" sec-type="COI-statement">
<title>Conflict of interest</title>
<p>The author(s) declared that this work was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p></sec>
<sec id="s10" sec-type="ai-statement">
<title>Generative AI statement</title>
<p>The author(s) declared that generative AI was not used in the creation of this manuscript.</p>
<p>Any alternative text (alt text) provided alongside figures in this article has been generated by Frontiers with the support of artificial intelligence and reasonable efforts have been made to ensure accuracy, including review by the authors wherever possible. If you identify any issues, please contact us.</p></sec>
<sec id="s11" sec-type="disclaimer">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p></sec>
<ref-list>
<title>References</title>
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