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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Plant Sci.</journal-id>
<journal-title>Frontiers in Plant Science</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Plant Sci.</abbrev-journal-title>
<issn pub-type="epub">1664-462X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fpls.2022.1093671</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Plant Science</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Research on a nondestructive model for the detection of the nitrogen content of tomato</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Zhang</surname><given-names>Xiaodong</given-names>
</name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<uri xlink:href="https://loop.frontiersin.org/people/1984192"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Duan</surname><given-names>Chaohui</given-names>
</name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Wang</surname><given-names>Yafei</given-names>
</name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<uri xlink:href="https://loop.frontiersin.org/people/1309151"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Gao</surname><given-names>Hongyan</given-names>
</name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Hu</surname><given-names>Lian</given-names>
</name>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
<uri xlink:href="https://loop.frontiersin.org/people/926232"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Wang</surname><given-names>Xinzhong</given-names>
</name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<xref ref-type="author-notes" rid="fn001"><sup>*</sup></xref>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>College of Agricultural Engineering, Jiangsu University</institution>, <addr-line>Zhenjiang</addr-line>, <country>China</country></aff>
<aff id="aff2"><sup>2</sup><institution>Key Laboratory of Modern Agricultural Equipment and Technology, Ministry of Education, Jiangsu University</institution>, <addr-line>Zhenjiang, Jiangsu</addr-line>, <country>China</country></aff>
<aff id="aff3"><sup>3</sup><institution>Key Laboratory of Key Technology on Agricultural Machine and Equipment, Ministry of Education, South China Agricultural University</institution>, <addr-line>Guangzhou</addr-line>, <country>China</country></aff>
<author-notes>
<fn fn-type="edited-by">
<p>Edited by: Jianfeng Ping, Zhejiang University, China</p>
</fn>
<fn fn-type="edited-by">
<p>Reviewed by: Fu Zhang, Henan University of Science and Technology, China; Jin Hu, Northwest A&amp;F University, China; Jingjin Zhang, Shanghai Jiao Tong University, China; Jun Ni, Nanjing Agricultural University, China</p>
</fn>
<fn fn-type="corresp" id="fn001">
<p>*Correspondence: Xinzhong Wang, <email xlink:href="mailto:xzwang@ujs.edu.cn">xzwang@ujs.edu.cn</email>
</p>
</fn>
<fn fn-type="other" id="fn002">
<p>This article was submitted to Sustainable and Intelligent Phytoprotection, a section of the journal Frontiers in Plant Science</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>11</day>
<month>01</month>
<year>2023</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>13</volume>
<elocation-id>1093671</elocation-id>
<history>
<date date-type="received">
<day>09</day>
<month>11</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>19</day>
<month>12</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2023 Zhang, Duan, Wang, Gao, Hu and Wang</copyright-statement>
<copyright-year>2023</copyright-year>
<copyright-holder>Zhang, Duan, Wang, Gao, Hu and Wang</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>The timely detection of information on crop nutrition is of great significance for improving the production efficiency of facility crops. In this study, the terahertz (THz) spectral information of tomato plant leaves with different nitrogen levels was obtained. The noise reduction of the THz spectral data was then carried out by using the Savitzky-Golay (S-G) smoothing algorithm. The sample sets were then analyzed by using Kennard-Stone (KS) and random sampling (RS) methods, respectively. The KS algorithm was optimized to divide the sample sets. The stability competitive adaptive reweighted sampling (SCARS), uninformative variable elimination (UVE), and interval partial least-squares (iPLS) algorithms were then used to screen the pre-processed THz spectral data. Based on the selected characteristic frequency bands, a model for the detection of the nitrogen content of tomato based on the THz spectrum was established by the radial basis function neural network (RBFNN) and backpropagation neural network (BPNN) algorithms, respectively. The results show that the root-mean-square error of correction (RMSEC) and root-mean-square error of prediction (RMSEP) of the BPNN model were respectively 0.1722% and 0.1843%, and the determination coefficients of the correction set (<italic>R<sub>c</sub>
</italic><sup>2</sup>) and prediction set (<italic>R<sub>p</sub>
</italic><sup>2</sup>) were respectively 0.8447 and 0.8375. The RMSEC and RMSEP values of the RBFNN model were respectively 0.1322% and 0.1855%, and the <italic>R<sub>c</sub>
</italic><sup>2</sup> and <italic>R<sub>p</sub>
</italic><sup>2</sup> values were respectively 0.8714 and 0.8463. Thus, the accuracy of the model established by the RBFNN algorithm was slightly higher. Therefore, the nitrogen content of tomato leaves can be detected by THz spectroscopy. The results of this study can provide a theoretical basis for the research and development of equipment for the detection of the nitrogen content of tomato leaves.</p>
</abstract>
<kwd-group>
<kwd>terahertz spectroscopy</kwd>
<kwd>tomato</kwd>
<kwd>N</kwd>
<kwd>characteristic band</kwd>
<kwd>nondestructive detection</kwd>
</kwd-group>
<counts>
<fig-count count="18"/>
<table-count count="4"/>
<equation-count count="8"/>
<ref-count count="30"/>
<page-count count="14"/>
<word-count count="5850"/>
</counts>
</article-meta>
</front>
<body>
<sec id="s1" sec-type="intro">
<label>1</label>
<title>Introduction</title>
<p>China is the world&#x2019;s largest tomato-planting country, accounting for about 1/3 of the global tomato-planting area (<xref ref-type="bibr" rid="B24">Wang et&#xa0;al., 2021</xref>). At present, the planted area of facility tomato in China is in a leading position globally, but there is a large gap between the per-mu yield of facility tomato in China and that in developed countries. The main reason for this is that China has some long-term problems growing crops. The misuse of fertilizer during production leads to soil pollution, and a lack of a timely understanding of the nutritional status of crops leads to shortages of nutrients and the water supply during the fertilizer season (<xref ref-type="bibr" rid="B13">Li et&#xa0;al., 2019</xref>; <xref ref-type="bibr" rid="B11">Hu and Cai, 2021</xref>). Therefore, to improve the production efficiency of facility crops and avoid environmental problems caused by the unreasonable application of chemical fertilizers, it is necessary to carry out scientific and theoretical research on the detection of information on crop nutrition. This is expected to greatly improve the production efficiency of facility crops and reduce pollution. Thus, technology for the non-destructive testing of crop nutrition is of great significance.</p>
<p>In the traditional facility nutrition management process, the judgment of the nutritional status of plants is mainly realized by expert experience and chemical determination, which are characterized by some problems. Expert experience is easily affected by subjective factors, and accurate judgment cannot be achieved (<xref ref-type="bibr" rid="B3">Fitzgerald et&#xa0;al., 2006</xref>; <xref ref-type="bibr" rid="B10">Huang et&#xa0;al., 2009</xref>; <xref ref-type="bibr" rid="B27">Zhang et&#xa0;al., 2018</xref>). Although chemical determination has high detection accuracy, it is difficult to realize the dynamic feedback control of crop nutrition information due to poor timeliness, and the sampling process causes certain damage to crops (<xref ref-type="bibr" rid="B5">Gao et&#xa0;al., 2012</xref>; <xref ref-type="bibr" rid="B23">Tian et&#xa0;al., 2016</xref>).</p>
<p>In recent years, non-destructive testing technology has been used to diagnose the nutritional elements of crops. This technology can quickly judge the nutritional status of crops without causing damage to them, and has gradually become a popular method for nutritional testing (<xref ref-type="bibr" rid="B22">Song et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B26">Yang et&#xa0;al., 2018</xref>). Some research has been conducted on the nutritional element diagnosis of crops both domestically and internationally, and some achievements have been made; however, there remain some shortcomings. For example, the method of crop information processing is relatively simple, and the model accuracy is not high (<xref ref-type="bibr" rid="B25">Yada et&#xa0;al., 2008</xref>; <xref ref-type="bibr" rid="B8">Hang et&#xa0;al., 2015</xref>). Moreover, related research is mainly focused on the analysis of the reflection intensity, texture, and other characteristics of the crop leaves, and biological macromolecules inside crops, such as nucleic acids and phospholipids, cannot be detected in detail (<xref ref-type="bibr" rid="B1">Breitenstein et&#xa0;al., 2012</xref>; <xref ref-type="bibr" rid="B6">Gente et&#xa0;al., 2013</xref>; <xref ref-type="bibr" rid="B7">Gente et&#xa0;al., 2015</xref>).</p>
<p>Terahertz (THz) detection technology an advanced technology known as &#x201c;one of the ten technologies that will affect the future of mankind in the 21<sup>st</sup> century,&#x201d; and has received increasing attention in the biological sciences field (<xref ref-type="bibr" rid="B30">Zhao et&#xa0;al., 2018</xref>; <xref ref-type="bibr" rid="B28">Zhang et&#xa0;al., 2021</xref>). THz waves refer to electromagnetic waves with a frequency between 0.1 and 10 THz and a position between microwave and infrared radiation. Under THz radiation, the chemical bonds of the molecules of various nutrients are broken and formed within picoseconds, resulting in the strong absorption of THz waves. Thus, THz spectroscopy can be used for the detection of the nitrogen content of crops. While THz spectroscopy has been widely used, due to the limitations of detection objects and technical means, its application in the field of agricultural engineering remains in its infancy. Some scholars have found that the spectral resolution of THz time-domain spectroscopy (THz-TDS) can be used to identify the composition of objects, and THz imaging technology can be used to identify nutrients such as chlorophyll, lutein, and the nitrogen-to-sugar ratio. Characteristic fingerprints lacking internal components and macromolecules can be used to diagnose the internal structure of crops with different nutrients (<xref ref-type="bibr" rid="B17">Liu et&#xa0;al., 2020</xref>; <xref ref-type="bibr" rid="B29">Zhang et&#xa0;al., 2022</xref>). For example, Liu et&#xa0;al. (<xref ref-type="bibr" rid="B15">Liu and Han, 2014</xref>) took advantage of the fact that the absorption of the THz spectra of proteins, amino acids, and other substances in biscuits is much less than that of water. They conducted respective model analyses on the frequency domain, refractive index, and absorption coefficient of THz spectral data, and obtained the best effect of the absorption coefficient model. <xref ref-type="bibr" rid="B19">Long et&#xa0;al. (2017)</xref> used a THz spectrometer to obtain the spectral data of leaves <italic>in vitro</italic> in a point-by-point scanning manner, and observed the differences of different water contents under image reconstruction. The regression prediction model was established according to the mean values in the time and frequency domains and the measured water content of the THz image of the leaf. These previous studies prove the feasibility of using THz spectroscopy to detect crop nutrition.</p>
<p>Therefore, in view of the current shortcomings, the advantages of THz imaging technology were used in this research for the identification of chlorophyll, lutein, the nitrogen-to-sugar ratio, and other nutritionally abundant internal components and characteristic fingerprints of macromolecules. The detection accuracy of the nitrogen content of tomato leaves is expected to be improved by using the algorithm to detect crop nutrition.</p>
</sec>
<sec id="s2" sec-type="materials|methods">
<label>2</label>
<title>Materials and methods</title>
<sec id="s2_1">
<label>2.1</label>
<title>Sample cultivation</title>
<p>The quality of the test sample cultivation has a direct impact on the test results. Therefore, in the process of sample cultivation, the influence of environmental factors should be minimized and the accuracy of the sample data should be improved. The experiment was carried out in a Venlo-type greenhouse (32.2&#xb0;N, 119.5&#xb0;E) at the Key Laboratory of Modern Agricultural Equipment and Technology, Ministry of Education, Jiangsu University. The environmental temperature of the greenhouse was maintained at 10.7-29.4&#xb0;C, and the relative humidity was 37.3%-87.9%. The test samples were 906 red tomatoes (Shanghai Changchong Tomato Seed Industry Co., Ltd.). Tomato seeds with large, plump grains and similar shapes were selected, and the selected seeds were placed in lightly salted water to screen out diseased seeds and sclerotia. Additionally, a 0.3&#xa0;m &#xd7; 0.6&#xa0;m black plastic plug tray was selected as the seedling-raising device. The seedling base was composed of vermiculite, perlite, and peat at a ratio of 1:3:1. The screened seeds were evenly sown in the plastic plug tray. After the seedlings had three true leaves, they were transplanted into a plastic round pot with a radius of 10.5&#xa0;cm and a height of 29&#xa0;cm. To achieve the purpose of soilless cultivation, perlite with strong root fixation was selected as the matrix. Each sample was repeated 30 times. During the experiment, the cultured tomato plants were watered with the Japanese Yamazaki nutrient solution formula (<xref ref-type="bibr" rid="B20">Mao et&#xa0;al., 2022</xref>). <xref ref-type="fig" rid="f1"><bold>Figure&#xa0;1</bold></xref> displays the sample cultivation and transplanting site.</p>
<fig id="f1" position="float">
<label>Figure&#xa0;1</label>
<caption>
<p>The sample cultivation. <bold>(A)</bold> Before smoothing <bold>(B)</bold> After smoothing.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g001.tif"/>
</fig>
</sec>
<sec id="s2_2">
<label>2.2</label>
<title>Equipment</title>
<p>The TS7400 THz&#x2013;TDS measurement system produced by Japan&#x2019;s ADVAN Corporation was used to collect the THz information of the samples. The system is specially customized for the detection of agricultural biological information. It has an attenuated total reflection (ATR) module and can perceive high water contents for the detection of biological tissue and living samples. <xref ref-type="fig" rid="f2"><bold>Figure&#xa0;2</bold></xref> shows the structure of the TS7400 THz-TDS measurement system.</p>
<fig id="f2" position="float">
<label>Figure&#xa0;2</label>
<caption>
<p>The structure and working principle of the Advantest-TS7400 THz-TDS measurement system.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g002.tif"/>
</fig>
<p>1. Operating/analyzing computers; 2. Ethernet; 3. Optical fiber; 4. Analysis unit; 5. Measurement unit; 6. THz transmitter; 7. THz detector; 8. Sample stage; 9. Cryostat transfer module; 10. Removable stand.</p>
<p>The working principle of the TS7400 THz-TDS measurement system is as follows. The THz measurement unit, the THz transmitter, and the THz detector are connected by optical fiber without adjusting the external optical path. The THz transmitter emits laser pulses that are divided into two mutually perpendicular beams under the action of the beam splitter. One laser beam is a stronger pump light, and the other is a weaker probe light. The pump light is incident on the emitting crystal to generate a THz pulse that passes through the sample stage through the mirror. It is then transmitted to the THz detector through the detection crystal collinear with the probe light that has undergone multiple reflections. The value is transmitted to the control computer. After the control computer receives the signal, the analysis unit can directly calculate parameters such as the refractive index, absorption coefficient, and dielectric constant of the sample, and the time-domain THz spectrum and distribution information of the sample can be obtained. Compared with the traditional THz device, this device not only has higher accuracy, but the size of the detectable sample is also expanded from a maximum of 3 cm&#xb2; to 225 cm&#xb2;, which can better meet the measurement needs of crop samples.</p>
</sec>
<sec id="s2_3">
<label>2.3</label>
<title>Sample data collection and processing</title>
<sec id="s2_3_1">
<label>2.3.1</label>
<title>Sample data collection</title>
<p>Samples were collected from the tomato plants after 65 days of nitrogen stress treatment. During leaf collection, the healthy 7-leaf pinnate compound leaves of the tomato that best reflect the growth state were selected and cut off. They were immediately placed in a sealed bag to maintain freshness, which was placed in a portable refrigerated incubator (<xref ref-type="bibr" rid="B21">Ni et&#xa0;al., 2021</xref>) to prevent the external environment from affecting it. Twenty leaf samples were selected for each nitrogen stress gradient, and a total of 80 samples were collected from four gradients. The samples were then placed in the THz-TDS measurement system for sample scanning to obtain the spectral information. Before the experiment, a dehumidifier was turned on, and the relative humidity in the sample detection box was reduced to below 5% to eliminate the interference of water vapor on the THz spectrum. Ten sampling points were scanned for each sample to obtain the spectral information, and the average value was taken as the data collected for the sample.</p>
<p>The nitrogen content of the collected test samples was determined by the Nessler reagent colorimetric method, and the colorimetry was performed with a spectrophotometer at 420 nm. The actual measurement value of the nitrogen content of the sample was calculated by drawing the standard curve of the nitrogen content concentration and the photometric values, as presented in <xref ref-type="fig" rid="f3"><bold>Figure&#xa0;3</bold></xref>.</p>
<fig id="f3" position="float">
<label>Figure&#xa0;3</label>
<caption>
<p>The standard curve of the nitrogen content.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g003.tif"/>
</fig>
</sec>
<sec id="s2_3_2">
<label>2.3.2</label>
<title>Data smoothing</title>
<p>The Savitzky-Golay (S-G) smoothing algorithm is a commonly used algorithm in data preprocessing due to its simple, fast, and easy-to-use process. The principle is to first take a window with an odd number of points in width, and to use the least-squares method for fitting <italic>via</italic> the translation of the window. The original value is then replaced with the fitted value of the midpoint of the window to achieve the smoothing of the data (<xref ref-type="bibr" rid="B30">Zhao et&#xa0;al., 2018</xref>). In this study, the S-G smoothing algorithm was used to preprocess the data, and the window width was 7 points/time. Taking the power spectrum data as an example, the comparison of the effect before and after the smoothing of the THz power spectrum is shown in <xref ref-type="fig" rid="f4"><bold>Figure&#xa0;4</bold></xref>. The results demonstrate that the algorithm can effectively reduce the interference signal and improve the modeling efficiency and model accuracy.</p>
<fig id="f4" position="float">
<label>Figure&#xa0;4</label>
<caption>
<p>The comparison of the THz power spectrum before and after smoothing. <bold>(A)</bold> Before smoothing, <bold>(B)</bold> After smoothing.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g004.tif"/>
</fig>
</sec>
<sec id="s2_3_3">
<label>2.3.3</label>
<title>Data set partitioning</title>
<p>The division of the sample set is the key to the applicability of the model. If the selected calibration set has good representativeness, the predictive ability of the model can be enhanced.</p>
<p>The random sampling (RS) algorithm is a simple method of randomly extracting samples regularly or irregularly from the entire sample set. A portion of the samples can be randomly selected as the prediction set until the sampling is full, and the remaining portion is used as the calibration set. The Kennard-Stone (KS) method was jointly proposed by Kennard and Stone (<xref ref-type="bibr" rid="B9">He et&#xa0;al., 2018</xref>), and its sample screening process of the calibration set is as follows. By calculating the Euclidean distance between two samples, the two samples with the largest distance enter the calibration set. The distance between the two selected samples is selected, the shortest distance among them is selected, and the sample corresponding to the longest distance among these shortest distances is entered into the calibration set. This method can ensure that the calibration set samples are evenly distributed according to the spatial distance, and the Euclidean distance between the two vectors is calculated as follows:</p>
<disp-formula>
<label>(1)</label>
<mml:math display="block" id="M1">
<mml:mrow>
<mml:msub>
<mml:mi>d</mml:mi>
<mml:mi>x</mml:mi>
</mml:msub>
<mml:mo stretchy="false">(</mml:mo>
<mml:mi>p</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>q</mml:mi>
<mml:mo stretchy="false">)</mml:mo>
<mml:mo>=</mml:mo>
<mml:msqrt>
<mml:mrow>
<mml:mstyle displaystyle="true">
<mml:munderover>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>j</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mi>J</mml:mi>
</mml:munderover>
<mml:mrow>
<mml:msup>
<mml:mrow>
<mml:mo stretchy="false">[</mml:mo>
<mml:msub>
<mml:mi>x</mml:mi>
<mml:mi>p</mml:mi>
</mml:msub>
<mml:mo stretchy="false">(</mml:mo>
<mml:mi>j</mml:mi>
<mml:mo stretchy="false">)</mml:mo>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mi>x</mml:mi>
<mml:mi>q</mml:mi>
</mml:msub>
<mml:mo stretchy="false">(</mml:mo>
<mml:mi>j</mml:mi>
<mml:mo stretchy="false">)</mml:mo>
<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 <italic>d</italic><sub><italic>x</italic>
</sub>(<italic>p</italic>,<italic>q</italic>) is the Euclidean distance of the spectral reflectance between samples <italic>p</italic> and <italic>q</italic>, is the reflectance of sample <italic>p</italic> at the <italic>j</italic><sup>th</sup> wavelength point, <italic>x</italic><sub><italic>q</italic>
</sub>(<italic>j</italic>) is the reflectance of <italic>q</italic> at the <italic>j</italic><sup>th</sup> wavelength the reflectivity of each wavelength point, and <italic>J</italic> is the number of wavelength points.</p>
<p>
<xref ref-type="table" rid="T1"><bold>Table&#xa0;1</bold></xref> reports the results of the power spectrum and absorbance after sample division by the RS and KS algorithms.</p>
<table-wrap id="T1" position="float">
<label>Table&#xa0;1</label>
<caption>
<p>The results of sample division by the RS and KS algorithms.</p>
</caption>
<table frame="hsides">
<tbody>
<tr>
<td valign="middle" align="left">Method</td>
<td valign="middle" align="center"><italic>R</italic><sup>2</sup>
</td>
<td valign="middle" align="center">RMSE</td>
</tr>
<tr>
<td valign="middle" align="left">RS</td>
<td valign="middle" align="center">0.8427</td>
<td valign="middle" align="center">0.1379</td>
</tr>
<tr>
<td valign="middle" align="left">KS</td>
<td valign="middle" align="center">0.8922</td>
<td valign="middle" align="center">0.1003</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The data in the calibration set obtained by sample division by the KS algorithm had a higher determination coefficient and a lower root-mean-square error (RMSE) than the data obtained by the RS algorithm. The subsequent data analysis and processing were therefore carried out on the basis of the division of the sample data set by the KS algorithm.</p>
</sec>
</sec>
<sec id="s2_4">
<label>2.4</label>
<title>Model construction method</title>
<sec id="s2_4_1">
<label>2.4.1</label>
<title>Uninformative variable elimination</title>
<p>Uninformative variable elimination (UVE) (<xref ref-type="bibr" rid="B12">Jiang et&#xa0;al., 2019</xref>) can filter out spectral variables that contribute less to the modeling, which allows for the selection of representative spectral variables. The filtered variables are called uninformative variables, and by filtering them out, the complexity of the model and the number of variables required for subsequent modeling can be reduced. The UVE algorithm is based on the partial least-squares (PLS) algorithm. During variable screening, artificial noise variables equal to the original variables are added to the PLS model. The variables are randomly numbered, and one is left by crossover. This method is used to obtain regression coefficients of variables including artificial noise. In the analysis, the random change generated by artificial noise is used as a reference, and the reliability of each variable is measured by the threshold and the stability value. When the absolute value of the stability is less than the threshold, the variables in this part are regarded as non-informative variables. The stability value is defined as follows:</p>
<disp-formula>
<label>(2)</label>
<mml:math display="block" id="M2">
<mml:mrow>
<mml:msub>
<mml:mi>S</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mi>m</mml:mi>
<mml:mi>e</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>n</mml:mi>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mi>b</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mrow>
<mml:mi>s</mml:mi>
<mml:mi>t</mml:mi>
<mml:mi>d</mml:mi>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mi>b</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mfrac>
<mml:mo>;</mml:mo>
<mml:mo>&#x2003;</mml:mo>
<mml:mi>i</mml:mi>
<mml:mo>=</mml:mo>
<mml:mn>1</mml:mn>
<mml:mo>,</mml:mo>
<mml:mn>2</mml:mn>
<mml:mo>,</mml:mo>
<mml:mn>3</mml:mn>
<mml:mo>&#x22ef;</mml:mo>
<mml:mo>,</mml:mo>
<mml:mi>m</mml:mi>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>i</italic> is the sample variable number, <italic>S</italic><sub>i</sub> is the stability value of the variable numbered <italic>i</italic>, <italic>b<sub>i</sub>
</italic> is the regression coefficient of the variable numbered <italic>i</italic>, <italic>std</italic>(<italic>b<sub>i</sub>
</italic>) is the regression coefficient of <italic>b<sub>i</sub>
</italic>, <italic>mean</italic>(<italic>b<sub>i</sub>
</italic>) is the mean value of <italic>b<sub>i</sub>
</italic>, and <italic>m</italic> is the total number of variables.</p>    <p>The steps of using the UVE algorithm to filter the feature frequencies are as follows.</p>
<list list-type="simple">
<list-item>
<p>(1) A <italic>&#x3bb;&#xd7;&#xb5;</italic> noise matrix is artificially generated, the spectral matrix is set as <italic>X</italic>, and the spectral matrix and noise matrix are spliced into a new matrix <italic>P</italic> of <italic>&#x3bb;</italic>&#xd7;2<italic>&#xb5;</italic>.</p>
</list-item>
<list-item>
<p>(2) Using the cross leave-one-out method, a regression analysis is performed on the matrix <italic>P</italic>, and the regression coefficient matrix <italic>L</italic> (<italic>&#x3bb;</italic>&#xd7;2<italic>&#xb5;</italic>) is obtained.</p>
</list-item>
<list-item>
<p>(3) The mean value <italic>mean</italic>(<italic>b<sub>i</sub>
</italic>) and the regression coefficient <italic>std</italic>(<italic>b<sub>i</sub>
</italic>) are respectively calculated, and the stability value matrix corresponding to each variable is obtained by Eq. (4).</p>
</list-item>
<list-item>
<p>(4) In the range of the noise variable interval [<italic>&#xb5;</italic>+1, 2<italic>&#xb5;</italic>], the maximum and minimum values of the stability value matrix are obtained, and the characteristic variable is selected in the range of [1, <italic>&#xb5;</italic>].</p>
</list-item>
</list>
</sec>
<sec id="s2_4_2">
<label>2.4.2</label>
<title>Stability competition adaptive reweighting sampling algorithm</title>
<p>Stability competitive adaptive reweighted sampling (SCARS) (<xref ref-type="bibr" rid="B18">Liu et&#xa0;al., 2014</xref>) is a common algorithm used to screen the optimal feature combination. During calculation, the measured THz spectral data can be set as a matrix <italic>X<sub>N&#xd7;P</sub>
</italic>. The number of samples is <italic>N</italic>, <italic>P</italic> is the number of variables, and the specific operation steps of SCARS are as follows.</p>
<p>(1) The stability value <italic>c<sub>j</sub>
</italic> of each frequency-band variable is calculated as follows:</p>
<disp-formula>
<label>, (3)</label>
<mml:math display="block" id="M3">
<mml:mrow>
<mml:msub>
<mml:mi>c</mml:mi>
<mml:mi>j</mml:mi>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mrow>
<mml:mo>|</mml:mo>
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>b</mml:mi>
<mml:mi>j</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mi>s</mml:mi>
<mml:mo stretchy="false">(</mml:mo>
<mml:msub>
<mml:mi>b</mml:mi>
<mml:mi>j</mml:mi>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
<mml:mo>|</mml:mo>
</mml:mrow>
<mml:mo>;</mml:mo>
<mml:mi>j</mml:mi>
<mml:mo>=</mml:mo>
<mml:mn>1</mml:mn>
<mml:mo>,</mml:mo>
<mml:mn>2</mml:mn>
<mml:mo>,</mml:mo>
<mml:mo>&#x22ef;</mml:mo>
<mml:mi>P</mml:mi>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>c<sub>j</sub>
</italic> is the stability value of the <italic>j</italic><sup>th</sup> variable during Monte Carlo (M) sampling, <italic>b<sub>j</sub>
</italic> is the value of the <italic>j</italic><sup>th</sup> variable during M sampling, and <italic>s(b<sub>j</sub>)</italic> is the standard deviation of the <italic>j</italic><sup>th</sup> variable during M sampling.</p>
<p>(2) The adaptive reweighted sampling method is combined with forced frequency band selection to screen groups with large stability values. They are combined into a subset of variables, and the ratio of variables to the whole frequency band is determined by the exponential decay function (EDF).</p>
<p>(3) These two steps are repeated in turn to obtain variable subset <italic>K</italic>. A PLS regression (PLSR) model is obtained, and the obtained variable subset is then evaluated through tenfold cross-validation. The <italic>K</italic> value is the number of operations in the SCARS algorithm, and the RMSE of cross-validation (RMSECV) value can be used as the judgment basis for whether the variable subset is a feature variable subset. The feature variable subset can be obtained at the smallest value of the RMSECV.</p>
</sec>
<sec id="s2_4_3">
<label>2.4.3</label>
<title>Interval partial least-squares algorithm</title>
<p>Interval PLS (iPLS) (<xref ref-type="bibr" rid="B2">De Lima et&#xa0;al., 2012</xref>) is a commonly used interval filtering algorithm for characteristic variables that was proposed by Norgaard at the beginning of the 20<sup>th</sup> century. Based on the PLSR model, the algorithm divides the overall intervals into equal intervals to be filtered. The PLSR model of each equally spaced interval <italic>n</italic> is respectively established. By comparing the model accuracy of each subinterval, the subinterval with the best accuracy is selected as the modeling candidate frequency interval.</p>
</sec>
<sec id="s2_4_4">
<label>2.4.4</label>
<title>Radial basis function neural network</title>
<p>Radial basis function neural networks (RBFNNs) are developed based on the multi-dimensional spatial interpolation of radial basis functions. They are feed-forward neural networks with good performance and can be understood as function approximation or curve fitting in high-dimensional space. The proposal of the RBFNN provided new ideas and methods for the application and research of neural networks in various fields. In practical applications, this neural network has the advantages of a fast learning speed, no local minimum problem, and the ability to establish a corresponding network topology according to different types of data (<xref ref-type="bibr" rid="B4">Gao et&#xa0;al., 2014</xref>).</p>
<p>The RBFNN is mainly composed of an input layer, a hidden layer, and an output layer. When using this neural network to establish the model, <italic>P</italic> can be set as the sample input matrix of the correction set, and <italic>T</italic> is the sample output matrix of the correction set. The calculation formula of hidden-layer neurons can be obtained as follows:</p>
<disp-formula>
<label>, (4)</label>
<mml:math display="block" id="M4">
<mml:mrow>
<mml:msub>
<mml:mi>a</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mi>exp</mml:mi>
<mml:mo stretchy="false">(</mml:mo>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mrow>
<mml:mo>&#x2016;</mml:mo>
<mml:mrow>
<mml:mi>C</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mo>&#x2016;</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:msub>
<mml:mi>b</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo stretchy="false">)</mml:mo>
<mml:mo>;</mml:mo>
<mml:mi>i</mml:mi>
<mml:mo>=</mml:mo>
<mml:mn>1</mml:mn>
<mml:mo>,</mml:mo>
<mml:mn>2</mml:mn>
<mml:mo>,</mml:mo>
<mml:mo>&#x22ef;</mml:mo>
<mml:mo>,</mml:mo>
<mml:mi>Q</mml:mi>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>Q</italic> is the number of calibration set samples, and <italic>C</italic> is the center of the radial basis function. The connection weight between the hidden layer and input layer is set as <italic>W</italic>. Moreover, <italic>b<sub>2</sub>
</italic> is the threshold value of <italic>N</italic> output layer neurons, and the following formula can be obtained.</p>
<disp-formula>
<label>(5)</label>
<mml:math display="block" id="M5">
<mml:mrow>
<mml:mrow>
<mml:mo>[</mml:mo>
<mml:mrow>
<mml:mi>W</mml:mi>
<mml:mo>;</mml:mo>
<mml:msub>
<mml:mi>b</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
</mml:mrow>
<mml:mo>]</mml:mo>
</mml:mrow>
<mml:mo>&#xd7;</mml:mo>
<mml:mrow>
<mml:mo>[</mml:mo>
<mml:mrow>
<mml:mi>A</mml:mi>
<mml:mo>;</mml:mo>
<mml:mi>I</mml:mi>
</mml:mrow>
<mml:mo>]</mml:mo>
</mml:mrow>
<mml:mo>=</mml:mo>
<mml:mi>T</mml:mi>
<mml:mo>;</mml:mo>
<mml:mi>A</mml:mi>
<mml:mo>=</mml:mo>
<mml:mrow>
<mml:mo>[</mml:mo>
<mml:mrow>
<mml:mi>a</mml:mi>
<mml:mn>1</mml:mn>
<mml:mo>,</mml:mo>
<mml:mi>a</mml:mi>
<mml:mn>2</mml:mn>
<mml:mo>,</mml:mo>
<mml:mo>&#x22ef;</mml:mo>
<mml:mo>,</mml:mo>
<mml:msub>
<mml:mi>a</mml:mi>
<mml:mi>Q</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mo>]</mml:mo>
</mml:mrow>
<mml:mo>;</mml:mo>
<mml:mi>I</mml:mi>
<mml:mo>=</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mrow>
<mml:mo>[</mml:mo>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>,</mml:mo>
<mml:mn>1</mml:mn>
<mml:mo>,</mml:mo>
<mml:mo>&#x22ef;</mml:mo>
<mml:mo>,</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mo>]</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:mi>Q</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</disp-formula>
<p>By solving Eq. (5), the threshold value <italic>b<sub>2</sub>
</italic> and the connection weight value <italic>W</italic> between the output layer and the hidden layer can be obtained as follows.</p>
<disp-formula>
<label>(6)</label>
<mml:math display="block" id="M6">
<mml:mrow>
<mml:mrow>
<mml:mo>{</mml:mo>
<mml:mtable columnalign="left">
<mml:mtr>
<mml:mtd>
<mml:mi>W</mml:mi>
<mml:mi>b</mml:mi>
<mml:mo>=</mml:mo>
<mml:mi>T</mml:mi>
<mml:mo stretchy="false">/</mml:mo>
<mml:mrow>
<mml:mo>[</mml:mo>
<mml:mrow>
<mml:mi>A</mml:mi>
<mml:mo>;</mml:mo>
<mml:mi>I</mml:mi>
</mml:mrow>
<mml:mo>]</mml:mo>
</mml:mrow>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd>
<mml:mi>W</mml:mi>
<mml:mo>=</mml:mo>
<mml:mi>W</mml:mi>
<mml:mi>b</mml:mi>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mo>:</mml:mo>
<mml:mo>,</mml:mo>
<mml:mn>1</mml:mn>
<mml:mo>:</mml:mo>
<mml:mi>Q</mml:mi>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd>
<mml:msub>
<mml:mi>b</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mi>W</mml:mi>
<mml:mi>b</mml:mi>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mo>;</mml:mo>
<mml:mo>,</mml:mo>
<mml:mi>Q</mml:mi>
<mml:mo>+</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:mrow>
</mml:mrow>
</mml:math>
</disp-formula>
</sec>
<sec id="s2_4_5">
<label>2.4.5</label>
<title>Backpropagation neural network</title>
<p>Backpropagation neural networks (BPNNs) (<xref ref-type="bibr" rid="B14">Li et&#xa0;al., 2020</xref>; <xref ref-type="bibr" rid="B16">Liu et&#xa0;al., 2021</xref>) can achieve the goal of not solving the relevant mapping equation in advance by learning the relationship between the input and output. Because of its high fault tolerance and parallel processing ability, the BPNN has a wide range of applications in target classification, recognition, and optimization.</p>    <p>The BPNN algorithm is mainly composed of forward calculation and error-reverse calculation. The topology includes an input layer, a hidden layer, and an output layer. During forward calculation, when the signal received by the output layer is an unexpected output value, a reverse propagation error signal will be generated, and the propagation path is the initial connection path. Compared with the RBFNN, the BPNN has the following characteristics.</p>
<list list-type="simple">
<list-item>
<p>(1) It has more hidden layers and hidden-layer nodes, and it can approximate any nonlinear mapping relationship.</p>
</list-item>
<list-item>
<p>(2) BPNNs are global approximation algorithms, which improves their generalization ability at the cost of reducing model accuracy.</p>
</list-item>
<list-item>
<p>(3) The ownership value must be updated during each sample learning. While this increases the robustness of the reverse neural network model, the update of the weight value slows down the convergence speed and the model easily falls into the local minimum.</p>
</list-item>
</list>
</sec>
</sec>
</sec>
<sec id="s3" sec-type="results">
<label>3</label>
<title>Results and discussion</title>
<p>To build the model for the prediction of the nitrogen content of tomato, all samples were divided into calibration and prediction sets. There were 80 samples to be tested, of which 60 were included in the calibration set and 20 were included in the prediction set. The RMSE was used to evaluate the fitting accuracy of the calibration set model, and the coefficient of determination (<italic>R</italic><sup>2</sup>) was used to examine the degree of correlation. Their calculation formulas are as follows:</p>
<disp-formula>
<label>(7)</label>
<mml:math display="block" id="M7">
<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:mrow>
<mml:mstyle displaystyle="true">
<mml:munderover>
<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:munderover>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mi>y</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mover>
<mml:mi>y</mml:mi>
<mml:mo>^</mml:mo>
</mml:mover>
</mml:mrow>
</mml:mstyle>
<mml:msup>
<mml:mo stretchy="false">)</mml:mo>
<mml:mn>2</mml:mn>
</mml:msup>
</mml:mrow>
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:msqrt>
</mml:mrow>
</mml:math>
</disp-formula>
<disp-formula>
<label>(8)</label>
<mml:math display="block" id="M8">
<mml:mrow>
<mml:msup>
<mml:mi>R</mml:mi>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>=</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mstyle displaystyle="true">
<mml:mo>&#x2211;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mover accent="true">
<mml:mi>y</mml:mi>
<mml:mo>^</mml:mo>
</mml:mover>
<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:mstyle>
</mml:mrow>
<mml:mrow>
<mml:mstyle displaystyle="true">
<mml:mo>&#x2211;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mover accent="true">
<mml:mi>y</mml:mi>
<mml:mo>^</mml:mo>
</mml:mover>
<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:mstyle>
</mml:mrow>
</mml:mfrac>
<mml:mo>=</mml:mo>
<mml:mn>1</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mstyle displaystyle="true">
<mml:mo>&#x2211;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mi>y</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mover accent="true">
<mml:mi>y</mml:mi>
<mml:mo>^</mml:mo>
</mml:mover>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mn>2</mml:mn>
</mml:msup>
</mml:mstyle>
</mml:mrow>
<mml:mrow>
<mml:mstyle displaystyle="true">
<mml:mo>&#x2211;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mi>y</mml:mi>
<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:mstyle>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>y</italic> is the measured value of the <italic>i</italic><sup>th</sup> sample in the calibration set, <italic>&#x177;</italic> is the predicted value of the <italic>i</italic><sup>th</sup> sample in the calibration set, and <italic>&#x233;</italic> is the average value of the measured values of all samples in the calibration set.</p>
<sec id="s3_1">
<label>3.1</label>
<title>Extraction of THz spectral information from tomato leaves</title>
<p>In the frequency-domain spectrum, with the change of the band, the samples have different absorptions of THz waves at different frequencies, as shown in <xref ref-type="fig" rid="f5"><bold>Figure&#xa0;5</bold></xref>. The figure presents the THz frequency-domain spectral curves of four different nitrogen-stressed tomato leaf samples, from which it is evident that the trends of various spectral curves were roughly similar.</p>
<fig id="f5" position="float">
<label>Figure&#xa0;5</label>
<caption>
<p>The THz frequency-domain spectra of leaf samples with different nitrogen contents.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g005.tif"/>
</fig>
<p>By preprocessing the raw THz spectral data, the vast majority of invalid information and noise signals in the data were removed. It can also be seen from <xref ref-type="fig" rid="f5"><bold>Figure&#xa0;5</bold></xref> that there were obvious gradient differences in the THz power spectrum curves of the samples under different nitrogen stress gradients. In the power spectrum graph, the value of the power spectrum shows a trend of first increasing and then decreasing, and it reached a peak value of around 0.7 THz. At the peak value and its surrounding frequencies, the nitrogen stress gradient curves presented obvious stratification. However, when the frequency was too small or too large, the THz power spectrum of each stress gradient was too dense, and the discrimination was not obvious.</p>
<sec id="s3_1_1">
<label>3.1.1</label>
<title>Processing results of the uninformative variable removal algorithm</title>
<p>
<xref ref-type="fig" rid="f6"><bold>Figure&#xa0;6</bold></xref> shows the results of the uninformative variable screening.</p>
<fig id="f6" position="float">
<label>Figure&#xa0;6</label>
<caption>
<p>The UVE feature frequency point screening results.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g006.tif"/>
</fig>
<p>In <xref ref-type="fig" rid="f6"><bold>Figure&#xa0;6</bold></xref>, the left side is the THz spectrum variable, the right side is the artificially generated noise variable, and the abscissa and the ordinate are respectively the serial number and stability index corresponding to the variable. The larger the absolute value of the stability index corresponding to the variable, the greater the correlation with the model. The dotted line in the figure is the screening threshold set based on artificial noise. Based on this threshold, a total of 17 characteristic frequency bands were screened, as shown in <xref ref-type="fig" rid="f7"><bold>Figures&#xa0;7</bold></xref>, <xref ref-type="fig" rid="f8"><bold>8</bold></xref>.</p>
<fig id="f7" position="float">
<label>Figure&#xa0;7</label>
<caption>
<p>The characteristic bands selected based on the UVE algorithm.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g007.tif"/>
</fig>
<fig id="f8" position="float">
<label>Figure&#xa0;8</label>
<caption>
<p>THz images of leaves with different nitrogen levels in the characteristic frequency bands screened by the UVE algorithm.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g008.tif"/>
</fig>
</sec>
<sec id="s3_1_2">
<label>3.1.2</label>
<title>Processing results for the stability competition adaptive reweighting sampling algorithm</title>
<p>In this study, when using the SCARS algorithm for filtering, the number of cycle sampling instances was 50 and THz power spectrum data were taken as the object. After 50 rounds of sampling had been reached, each index value had reached a stable state. The processing result of the SCARS algorithm is shown in <xref ref-type="fig" rid="f9"><bold>Figure&#xa0;9</bold></xref>.</p>
<fig id="f9" position="float">
<label>Figure&#xa0;9</label>
<caption>
<p>The running process of the SCARS algorithm.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g009.tif"/>
</fig>
<p>It can be seen from <xref ref-type="fig" rid="f9"><bold>Figure&#xa0;9</bold></xref> that with the increase of the number of iterations of the SCARS algorithm, the number of frequency bands retained generally decreased. However, the speed of reduction slowed down, indicating that the SCARS algorithm used coarse screening in the early stages of screening the characteristic frequency bands and fine screening in the later stages. It can be seen that with the gradual increase of the number of runs, the RMSECV value presented a decreasing trend. The RMSECV value was the minimum when the number of runs reached 43, which indicates that the frequency band with less correlation with the sample nitrogen content had been removed before. After 43 runs, the value had rebounded, and, combined with the change in the regression coefficient path, this indicates that the characteristic frequency bands related to the sample nitrogen content may have been removed by mistake. When the RMSECV value was the lowest, the subset of selected characteristic frequency bands was the best. Five characteristic frequencies were obtained, namely 0.574, 0.624, 0.642, 0.704, and 0.817 THz, and they were used as alternative characteristic frequency bands. The selected THz spectral bands are shown in <xref ref-type="fig" rid="f10"><bold>Figures&#xa0;10</bold></xref>, <xref ref-type="fig" rid="f11"><bold>11</bold></xref>.</p>
<fig id="f10" position="float">
<label>Figure&#xa0;10</label>
<caption>
<p>The characteristic bands selected based on the SCARS algorithm.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g010.tif"/>
</fig>
<fig id="f11" position="float">
<label>Figure&#xa0;11</label>
<caption>
<p>THz images of leaves with different nitrogen levels in the characteristic frequency bands screened by the SCARS algorithm.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g011.tif"/>
</fig>
</sec>
<sec id="s3_1_3">
<label>3.1.3</label>
<title>Processing results for the interval partial least squares algorithm</title>
<p>When using the iPLS algorithm to filter the optimal frequency band interval, the number of subintervals to be divided must first be determined. Too many or too few subintervals will affect the subsequent selection of the optimal frequency band interval. In this study, the pretreated THz spectral intervals were divided into 10-45 equidistant intervals. As shown in <xref ref-type="fig" rid="f12"><bold>Figure&#xa0;12</bold></xref>, when the RMSECV value was the minimum, the overall THz spectral interval was divided into 22 equidistant subintervals.</p>
<fig id="f12" position="float">
<label>Figure&#xa0;12</label>
<caption>
<p>The results of the optimal number of isometric interval partitions.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g012.tif"/>
</fig>
<p>According to the number of subintervals shown in <xref ref-type="fig" rid="f12"><bold>Figure&#xa0;12</bold></xref>, the THz spectral interval in the range of 0-1.4 THz was divided into 22 equal parts, and the PLS model index values in each subinterval were calculated. <xref ref-type="table" rid="T2"><bold>Table&#xa0;2</bold></xref> reports the THz spectral frequency division range of each subinterval and the corresponding RMSECV value. <xref ref-type="fig" rid="f13"><bold>Figures&#xa0;13</bold></xref>, <xref ref-type="fig" rid="f14"><bold>14</bold></xref> show the operation results of the iPLS algorithm.</p>
<table-wrap id="T2" position="float">
<label>Table&#xa0;2</label>
<caption>
<p>The index values of each subinterval model.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" align="left">Number</th>
<th valign="middle" align="center">Frequency range (THz)</th>
<th valign="middle" align="center">RMSECV (%)</th>
<th valign="middle" align="center">Number</th>
<th valign="middle" align="center">Frequency range (THz)</th>
<th valign="middle" align="center">RMSECV (%)</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="left">1</td>
<td valign="middle" align="center">0-0.0636</td>
<td valign="middle" align="center">0.8641</td>
<td valign="middle" align="center">12</td>
<td valign="middle" align="center">0.6996-0.7632</td>
<td valign="middle" align="center">0.3671</td>
</tr>
<tr>
<td valign="middle" align="left">2</td>
<td valign="middle" align="center">0.0636 ~0.1272</td>
<td valign="middle" align="center">0.8327</td>
<td valign="middle" align="center">13</td>
<td valign="middle" align="center">0.7632-0.8268</td>
<td valign="middle" align="center">0.3826</td>
</tr>
<tr>
<td valign="middle" align="left">3</td>
<td valign="middle" align="center">0.1272-0.1908</td>
<td valign="middle" align="center">0.7874</td>
<td valign="middle" align="center">14</td>
<td valign="middle" align="center">0.8268-0.8904</td>
<td valign="middle" align="center">0.4952</td>
</tr>
<tr>
<td valign="middle" align="left">4</td>
<td valign="middle" align="center">0.1908-0.2544</td>
<td valign="middle" align="center">0.8234</td>
<td valign="middle" align="center">15</td>
<td valign="middle" align="center">0.8904-0.9540</td>
<td valign="middle" align="center">0.4611</td>
</tr>
<tr>
<td valign="middle" align="left">5</td>
<td valign="middle" align="center">0.2544-0.3180</td>
<td valign="middle" align="center">0.7851</td>
<td valign="middle" align="center">16</td>
<td valign="middle" align="center">0.9540-1.0176</td>
<td valign="middle" align="center">0.5312</td>
</tr>
<tr>
<td valign="middle" align="left">6</td>
<td valign="middle" align="center">0.3180-0.3816</td>
<td valign="middle" align="center">0.7687</td>
<td valign="middle" align="center">17</td>
<td valign="middle" align="center">1.0176-1.0812</td>
<td valign="middle" align="center">0.6074</td>
</tr>
<tr>
<td valign="middle" align="left">7</td>
<td valign="middle" align="center">0.3816-0.4452</td>
<td valign="middle" align="center">0.7002</td>
<td valign="middle" align="center">18</td>
<td valign="middle" align="center">1.0812-1.1448</td>
<td valign="middle" align="center">0.6341</td>
</tr>
<tr>
<td valign="middle" align="left">8</td>
<td valign="middle" align="center">0.4452-0.5088</td>
<td valign="middle" align="center">0.6784</td>
<td valign="middle" align="center">19</td>
<td valign="middle" align="center">1.1448-1.2084</td>
<td valign="middle" align="center">0.6139</td>
</tr>
<tr>
<td valign="middle" align="left">9</td>
<td valign="middle" align="center">0.5088-0.5724</td>
<td valign="middle" align="center">0.6174</td>
<td valign="middle" align="center">20</td>
<td valign="middle" align="center">1.2084-1.2720</td>
<td valign="middle" align="center">0.6732</td>
</tr>
<tr>
<td valign="middle" align="left">10</td>
<td valign="middle" align="center">0.5724-0.6360</td>
<td valign="middle" align="center">0.5412</td>
<td valign="middle" align="center">21</td>
<td valign="middle" align="center">1.2720-1.3356</td>
<td valign="middle" align="center">0.6954</td>
</tr>
<tr>
<td valign="middle" align="left">11</td>
<td valign="middle" align="center">0.6360-0.6996</td>
<td valign="middle" align="center">0.4317</td>
<td valign="middle" align="center">22</td>
<td valign="middle" align="center">1.3356-1.4000</td>
<td valign="middle" align="center">0.7441</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="f13" position="float">
<label>Figure&#xa0;13</label>
<caption>
<p>The results of running the iPLS algorithm.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g013.tif"/>
</fig>
<fig id="f14" position="float">
<label>Figure&#xa0;14</label>
<caption>
<p>THz images of leaves with different nitrogen levels in the characteristic frequency bands screened by the iPLS algorithm.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g014.tif"/>
</fig>
<p>It can be seen from <xref ref-type="fig" rid="f13"><bold>Figure&#xa0;13</bold></xref> that the index values of the PLS model established in each subinterval presented a trend of first decreasing and then increasing, and were closely related to the power spectrum curves of each stress gradient. When the power spectrum curve density was large, the corresponding modeling effect was poor; on the contrary, the modeling effect was better. Finally, the subinterval with the interval number of 12 was selected as the characteristic frequency subinterval, and there were 31 characteristic frequency points in total.</p>
</sec>
</sec>
<sec id="s3_2">
<label>3.2</label>
<title>Establishment and analysis of the model</title>
<sec id="s3_2_1" sec-type="results">
<label>3.2.1</label>
<title>Results for the radial basis function neural network</title>
<p>An RBFNN with strict logic was established by using the function package in MATLAB software. The expansion speed is the key to determining the quality of the RBFNN, and the setting of this parameter depends on the target object. <xref ref-type="fig" rid="f15"><bold>Figure&#xa0;15</bold></xref> exhibits the change of the RMSE of correction (RMSEC) of the RBFNN, iPLS, UVE, and SCARS models with an expansion speed of 0.1-1 and an interval of 0.1.</p>
<fig id="f15" position="float">
<label>Figure&#xa0;15</label>
<caption>
<p>The influence of the diffusion velocity on the RBFNN model.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g015.tif"/>
</fig>
<p>It can be seen from <xref ref-type="fig" rid="f15"><bold>Figure&#xa0;15</bold></xref> that when the diffusion speed was 0.5 and 0.6, the RBFNN model had the best RMSEC value. The established neural network model was tested to verify the prediction set, and the prediction results are reported in <xref ref-type="table" rid="T3"><bold>Table&#xa0;3</bold></xref>.</p>
<table-wrap id="T3" position="float">
<label>Table&#xa0;3</label>
<caption>
<p>The prediction results of the RBFNN model based on the THz spectrum.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" align="left">Algorithm for band screening</th>
<th valign="middle" align="center">RMSEC (%)</th>
<th valign="middle" align="center"><italic>R</italic><sub>c</sub><sup>2</sup>
</th>
<th valign="middle" align="center">RMSEP (%)</th>
<th valign="middle" align="center"><italic>R</italic><sub>p</sub><sup>2</sup>
</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="left">UVE</td>
<td valign="middle" align="center">0.1721</td>
<td valign="middle" align="center">0.8457</td>
<td valign="middle" align="center">0.2197</td>
<td valign="middle" align="center">0.8218</td>
</tr>
<tr>
<td valign="middle" align="left">SCARS</td>
<td valign="middle" align="center">0.1322</td>
<td valign="middle" align="center">0.8714</td>
<td valign="middle" align="center">0.1855</td>
<td valign="middle" align="center">0.8463</td>
</tr>
<tr>
<td valign="middle" align="left">iPLS</td>
<td valign="middle" align="center">0.2214</td>
<td valign="middle" align="center">0.8352</td>
<td valign="middle" align="center">0.2784</td>
<td valign="middle" align="center">0.8149</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>According to the results reported in <xref ref-type="table" rid="T3"><bold>Table&#xa0;3</bold></xref>, when the RBFNN algorithm was combined with the characteristic bands screened by SCARS, the detection model had the best effect. The RMSEC and the RMSE of prediction (RMSEP) were respectively 0.1322% and 0.1855%, and the determination coefficients of the correction set (<italic>R</italic><sub>c</sub><sup>2</sup>) and prediction set (<italic>R</italic><sub>p</sub><sup>2</sup>) were respectively 0.8714 and 0.8463. The scatter plot of the optimal results of the model based on the RBFNN algorithm is presented in <xref ref-type="fig" rid="f16"><bold>Figure&#xa0;16</bold></xref>.</p>
<fig id="f16" position="float">
<label>Figure&#xa0;16</label>
<caption>
<p>The scatter plot of the prediction results of the RBFNN model based on THz spectroscopy.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g016.tif"/>
</fig>
</sec>
<sec id="s3_2_2" sec-type="results">
<label>3.2.2</label>
<title>Results for the backpropagation neural network</title>
<p>The sample data were trained using the scaled conjugate gradient function in the BPNN tool in MATLAB software. The specific training process included using the newff function to construct the basic structure of the BPNN. Moreover, the architecture based on the BPNN trained the model through the Trainlm function, and the Sim function output model was used to train the process. Taking the combination of characteristic bands screened by the iPLS algorithm as an example, the training process of its BPNN is shown in <xref ref-type="fig" rid="f17"><bold>Figure&#xa0;17</bold></xref>.</p>
<fig id="f17" position="float">
<label>Figure&#xa0;17</label>
<caption>
<p>The training process of the BPNN model.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g017.tif"/>
</fig>
<p>It can be seen from <xref ref-type="fig" rid="f17"><bold>Figure&#xa0;17</bold></xref> that the number of network iterations epochs was 22. Moreover, the learning rate was set to 0.01, and the number of hidden-layer neurons was set to 6. The sample data filtered by other algorithms were input into the network after normalization, and the training results are reported in <xref ref-type="table" rid="T4"><bold>Table&#xa0;4</bold></xref>. By comparing the results in the table, it is evident that the modeling effect obtained by combining the SCARS filtering algorithm was the best.</p>
<table-wrap id="T4" position="float">
<label>Table&#xa0;4</label>
<caption>
<p>The prediction results of the BPNN model based on THz spectroscopy.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" align="left">Algorithm for band screening</th>
<th valign="middle" align="center">RMSEC (%)</th>
<th valign="middle" align="center"><italic>R</italic><sub>c</sub><sup>2</sup>
</th>
<th valign="middle" align="center">RMSEP (%)</th>
<th valign="middle" align="center"><italic>R</italic><sub>p</sub><sup>2</sup>
</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="left">iPLS</td>
<td valign="middle" align="center">0.2641</td>
<td valign="middle" align="center">0.8114</td>
<td valign="middle" align="center">0.2851</td>
<td valign="middle" align="center">0.8024</td>
</tr>
<tr>
<td valign="middle" align="left">UVE</td>
<td valign="middle" align="center">0.2148</td>
<td valign="middle" align="center">0.8322</td>
<td valign="middle" align="center">0.2363</td>
<td valign="middle" align="center">0.8187</td>
</tr>
<tr>
<td valign="middle" align="left">SCARS</td>
<td valign="middle" align="center">0.1721</td>
<td valign="middle" align="center">0.8447</td>
<td valign="middle" align="center">0.1843</td>
<td valign="middle" align="center">0.8375</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>According to the results reported in <xref ref-type="table" rid="T4"><bold>Table&#xa0;4</bold></xref>, when the BPNN algorithm was combined with the characteristic bands screened by SCARS, the RMSE values of the correction and prediction sets were respectively 0.1721% and 0.1843%, and the <italic>R</italic><sup>2</sup> values of the correction and prediction sets were respectively 0.8447 and 0.8375. The scatter plot of the optimal results of the BPNN model is shown in <xref ref-type="fig" rid="f18"><bold>Figure&#xa0;18</bold></xref>.</p>
<fig id="f18" position="float">
<label>Figure&#xa0;18</label>
<caption>
<p>The scatter plot of the prediction results of the BPNN model based on THz spectroscopy.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fpls-13-1093671-g018.tif"/>
</fig>
<p>The analysis of the nitrogen detection model based on the THz spectrum shows that the models built by the two algorithms had good prediction effects. In terms of accuracy, the RBFNN model was slightly better than the BPNN model.</p>
</sec>
</sec>
</sec>
<sec id="s4" sec-type="conclusions">
<label>4</label>
<title>Conclusion</title>    <p>In this study, a method for the detection of the nitrogen content of tomato based on THz spectroscopy was investigated. The basic contents of the method include data preprocessing, sample set division, characteristic frequency band screening, and model establishment. The research conclusions are as follows.</p>
<list list-type="simple">
<list-item>
<p>(1) In combination with the S-G smoothing algorithm, the original THz spectral data were denoised to remove invalid and interference information. The advantages and disadvantages of the KS and RS sample set partitioning algorithms were compared and analyzed. By analyzing the results of sample partitioning, it was concluded that the sample set divided by the KS algorithm could effectively cover the entire sample range, and the partitioning effect was the best.</p>
</list-item>
<list-item>
<p>(2) After noise reduction, the THz spectral data still relied on more low-correlation information. To improve the accuracy and efficiency of the model, the candidate characteristic bands of the THz spectrum were screened by using the UVE, SCARS, and iPLS algorithms, respectively.</p>
</list-item>
<list-item>
<p>(3) Based on the characteristic frequency bands screened by the iPLS, UVE, and SCARS algorithms, the RBFNN and BPNN algorithms were used to establish the models for the detection of the nitrogen content of tomatoes. The RMSEC and RMSEP values of the BPNN model were respectively 0.1722% and 0.1843%, and the determination <italic>R<sub>c</sub>
</italic><sup>2</sup> and <italic>R<sub>p</sub>
</italic><sup>2</sup> values were respectively 0.8447 and 0.8375. The RMSEC and RMSEP values of the RBFNN were respectively 0.1322% and 0.1855%, and its <italic>R<sub>c</sub>
</italic><sup>2</sup> and <italic>R<sub>p</sub>
</italic><sup>2</sup> values were respectively 0.8714 and 0.8463. Thus, the accuracy of the model established by the RBFNN algorithm was slightly higher.</p>
</list-item>
</list>
</sec>
<sec id="s5" sec-type="data-availability">
<title>Data availability statement</title>
<p>The original contributions presented in the study are included in the article/supplementary material. Further inquiries can be directed to the corresponding author.</p>
</sec>
<sec id="s6" sec-type="author-contributions">
<title>Author contributions</title>
<p>Conceptualization, XZ, HG and XW; methodology, XZ, HG, LH and XW; formal analysis, CD, HG and YW data curation, XZ and CD writing&#x2014;original draft preparation, XZ, YW and HG writing&#x2014;review and editing, XZ and Y W. All authors contributed to the article and approved the submitted version.</p>
</sec>
</body>
<back>
<sec id="s7" sec-type="funding-information">
<title>Funding</title>
<p>This research was funded by Project of Agricultural Equipment Department of Jiangsu University (NZXB20210106). Key Laboratory of Modern Agricultural Equipment and Technology(Jiangsu University), Ministry of Education (Grant No. MAET202111). National Key Research and Development Program for Young Scientists (2022YFD2000013). Key Laboratory of Modern Agricultural Equipment and Technology (Ministry of Education), High-tech Key Laboratory of Agricultural Equipment and Intelligence of Jiangsu Province (Grant No. JNZ201901). Scientific and Technological Project of Henan Province (Grant No. 212102110029).The National Natural Science Foundation of China (61771224 and 32071905).</p>
</sec>
<sec id="s8" sec-type="COI-statement">
<title>Conflict of interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec id="s9" 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>
<ref id="B1">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Breitenstein</surname> <given-names>B.</given-names>
</name>
<name>
<surname>Scheller</surname> <given-names>M.</given-names>
</name>
<name>
<surname>Shakfa</surname> <given-names>M. K.</given-names>
</name>
<name>
<surname>Kinder</surname> <given-names>T.</given-names>
</name>
<name>
<surname>Mueller-Wirts</surname> <given-names>T.</given-names>
</name>
<name>
<surname>Koch</surname> <given-names>M.</given-names>
</name>
<etal/>
</person-group>. (<year>2012</year>). <article-title>Introducing terahertz technology into plant biology: A novel method to monitor changes in leaf water status</article-title>. <source>J. Appl. Bot. Food Quality-angewandte Botanik.</source> <volume>84</volume>, <fpage>158</fpage>&#x2013;<lpage>161</lpage>.</citation>
</ref>
<ref id="B2">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>De Lima</surname> <given-names>C. P.</given-names>
</name>
<name>
<surname>Backes</surname> <given-names>C.</given-names>
</name>
<name>
<surname>Fernandes</surname> <given-names>D. M.</given-names>
</name>
<name>
<surname>Santos</surname> <given-names>A. J. M.</given-names>
</name>
<name>
<surname>de Godoy</surname> <given-names>L. J. G.</given-names>
</name>
<name>
<surname>Boas</surname> <given-names>R. L. V.</given-names>
</name>
</person-group> (<year>2012</year>). <article-title>Leaves reflectance index of the bermuda grass to evaluate the nutritional status in nitrogen</article-title>. <source>Ciencia Rural.</source> <volume>42</volume>, <fpage>1568</fpage>&#x2013;<lpage>1574</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.1590/S0103-84782012005000062</pub-id>
</citation>
</ref>
<ref id="B3">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Fitzgerald</surname> <given-names>G. J.</given-names>
</name>
<name>
<surname>Rodriguez</surname> <given-names>D.</given-names>
</name>
<name>
<surname>Christensen</surname> <given-names>L. K.</given-names>
</name>
<name>
<surname>Belford</surname> <given-names>R.</given-names>
</name>
<name>
<surname>Sadras</surname> <given-names>V. O.</given-names>
</name>
<name>
<surname>Clarke</surname> <given-names>T. R.</given-names>
</name>
</person-group> (<year>2006</year>). <article-title>Spectral and thermal sensing for nitrogen and water status in rainfed and irrigated wheat environments</article-title>. <source>Precis. Agriculture.</source> <volume>7</volume>, <fpage>233</fpage>&#x2013;<lpage>248</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.1007/s11119-006-9011-z</pub-id>
</citation>
</ref>
<ref id="B4">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Gao</surname> <given-names>H. Y.</given-names>
</name>
<name>
<surname>Mao</surname> <given-names>H. P.</given-names>
</name>
<name>
<surname>Zhang</surname> <given-names>X. D.</given-names>
</name>
</person-group> (<year>2014</year>). <article-title>Measurement of nitrogen content in lettuce canopy using SpectroscopyCombined with BiPLS-GA-SPA and ELM</article-title>. <source>Spectrosc. Spectral Analysis.</source> <volume>36</volume>, <fpage>491</fpage>&#x2013;<lpage>495</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.3964/j.issn.1000-0593(2016)02-0491-05</pub-id>
</citation>
</ref>
<ref id="B5">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Gao</surname> <given-names>H. Y.</given-names>
</name>
<name>
<surname>Mao</surname> <given-names>H. P.</given-names>
</name>
<name>
<surname>Zhang</surname> <given-names>X. D.</given-names>
</name>
<name>
<surname>Sun</surname> <given-names>J.</given-names>
</name>
</person-group> (<year>2012</year>). <article-title>Water moisture diagnosis of tomato canopy based on multi-information fusion</article-title>. <source>Trans. Chin. Soc. Agric. Engineering.</source> <volume>28</volume>, <fpage>140</fpage>&#x2013;<lpage>144</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.3969/j.issn.1002-6819.2012.16.022</pub-id>
</citation>
</ref>
<ref id="B6">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Gente</surname> <given-names>R.</given-names>
</name>
<name>
<surname>Born</surname> <given-names>N.</given-names>
</name>
<name>
<surname>Voss</surname> <given-names>N.</given-names>
</name>
<name>
<surname>Sannemann</surname> <given-names>W.</given-names>
</name>
<name>
<surname>Leon</surname> <given-names>J.</given-names>
</name>
<name>
<surname>Koch</surname> <given-names>M.</given-names>
</name>
<etal/>
</person-group>. (<year>2013</year>). <article-title>Determination of leaf water content from terahertz time-domain spectroscopic data</article-title>. <source>J. Infrared Millimeter Terahertz Waves.</source> <volume>34</volume>, <fpage>316</fpage>&#x2013;<lpage>323</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.1007/s10762-013-9972-8</pub-id>
</citation>
</ref>
<ref id="B7">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Gente</surname> <given-names>R.</given-names>
</name>
<name>
<surname>Rehn</surname> <given-names>A.</given-names>
</name>
<name>
<surname>Koch</surname> <given-names>M.</given-names>
</name>
</person-group> (<year>2015</year>). <article-title>Contactless water status measurements on plants at 35 GHz</article-title>. <source>J. Infrared Millimeter Terahertz Waves.</source> <volume>36</volume>, <fpage>312</fpage>&#x2013;<lpage>317</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.1007/s10762-014-0127-3</pub-id>
</citation>
</ref>
<ref id="B8">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Hang</surname> <given-names>T.</given-names>
</name>
<name>
<surname>Mao</surname> <given-names>H. P.</given-names>
</name>
<name>
<surname>Zhang</surname> <given-names>X. D.</given-names>
</name>
<name>
<surname>Hu</surname> <given-names>J.</given-names>
</name>
</person-group> (<year>2015</year>). <article-title>Nondestructive testing of tomato growth information based on machine vision</article-title>. <source>J. Agric. Mechanization Res.</source> <volume>37</volume>, <fpage>192</fpage>&#x2013;<lpage>197</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.13427/j.cnki.njyi.2015.11.043</pub-id>
</citation>
</ref>
<ref id="B9">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>He</surname> <given-names>Z. H.</given-names>
</name>
<name>
<surname>Ma</surname> <given-names>Z. H.</given-names>
</name>
<name>
<surname>Li</surname> <given-names>M. C.</given-names>
</name>
<name>
<surname>Zhou</surname> <given-names>Y.</given-names>
</name>
</person-group> (<year>2018</year>). <article-title>Selection of a calibration sample subset by a semi-supervised method</article-title>. <source>J. near infrared spectroscopy.</source> <volume>26</volume> (<issue>2</issue>), <fpage>87</fpage>&#x2013;<lpage>94</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.1177/0967033518762437</pub-id>
</citation>
</ref>
<ref id="B10">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Huang</surname> <given-names>C. J.</given-names>
</name>
<name>
<surname>Han</surname> <given-names>L. J.</given-names>
</name>
<name>
<surname>Liu</surname> <given-names>X.</given-names>
</name>
<name>
<surname>Ma</surname> <given-names>L. J.</given-names>
</name>
</person-group> (<year>2009</year>). <article-title>Rapid measurement for moisture and calorific value of straw based on near infrared spectroscopy and local algor ithm</article-title>. <source>J. Infrared Millin. Waves</source> <volume>28</volume>, <fpage>184</fpage>&#x2013;<lpage>187</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.3321/j.issn:1001-9014.2009.03.007</pub-id>
</citation>
</ref>
<ref id="B11">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Hu</surname> <given-names>Q. F.</given-names>
</name>
<name>
<surname>Cai</surname> <given-names>J.</given-names>
</name>
</person-group> (<year>2021</year>). <article-title>Research of terahertz time-domain spectral identification based on deep learning</article-title>. <source>Spectrosc. Spectral Analysis.</source> <volume>41</volume>, <fpage>94</fpage>&#x2013;<lpage>99</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.3964/j.issn.1000-0593(2021)01-0094-06</pub-id>
</citation>
</ref>
<ref id="B12">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Jiang</surname> <given-names>Y. Y.</given-names>
</name>
<name>
<surname>Ge</surname> <given-names>H. Y.</given-names>
</name>
<name>
<surname>Zhang</surname> <given-names>Y.</given-names>
</name>
</person-group> (<year>2019</year>). <article-title>Detection of foreign bodies in grain with terahertz reflection imaging</article-title>. <source>Optik.</source> <volume>181</volume>, <fpage>1130</fpage>&#x2013;<lpage>1138</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.1016/j.ijleo.2018.12.066</pub-id>
</citation>
</ref>
<ref id="B13">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Li</surname> <given-names>H. H.</given-names>
</name>
<name>
<surname>Liu</surname> <given-names>H.</given-names>
</name>
<name>
<surname>Pang</surname> <given-names>J.</given-names>
</name>
<name>
<surname>Li</surname> <given-names>S.</given-names>
</name>
<name>
<surname>Cui</surname> <given-names>Y. S.</given-names>
</name>
<name>
<surname>Sun</surname> <given-names>J. S.</given-names>
</name>
</person-group> (<year>2019</year>). <article-title>Effects of water and nitrogen interaction on growth and nutrient accumulation of potted tomatoes</article-title>. <source>Trans. Chin. Soc. Agric. Machinery.</source> <volume>50</volume>, <fpage>272</fpage>&#x2013;<lpage>279</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.6041/j.issn.1000-1298.2019.09.032</pub-id>
</citation>
</ref>
<ref id="B14">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Li</surname> <given-names>X. Y.</given-names>
</name>
<name>
<surname>Ren</surname> <given-names>G. X.</given-names>
</name>
<name>
<surname>Fan</surname> <given-names>P. P.</given-names>
</name>
<name>
<surname>Liu</surname> <given-names>Y.</given-names>
</name>
<name>
<surname>Sun</surname> <given-names>Z. L.</given-names>
</name>
<name>
<surname>Hou</surname> <given-names>G. L.</given-names>
</name>
<etal/>
</person-group>. (<year>2020</year>). <article-title>Study on the calibration transfer of soil nutrient concentration from the hyperspectral camera to the normal spectrometer</article-title>. <source>J. Spectroscopy.</source> <volume>16</volume>, <fpage>1028</fpage>&#x2013;<lpage>1035</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.1155/2020/8137142</pub-id>
</citation>
</ref>
<ref id="B15">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Liu</surname> <given-names>H.</given-names>
</name>
<name>
<surname>Han</surname> <given-names>D. H.</given-names>
</name>
</person-group> (<year>2014</year>). <article-title>Quantitative detection of moisture content of biscuits by terahertz time-domain spectroscopy</article-title>. <source>J. Food Saf. Quality.</source> <volume>5</volume> (<issue>3</issue>), <fpage>725</fpage>&#x2013;<lpage>729</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.19812/j.cnki.jfsq11-5956/ts.2014.03.016</pub-id>
</citation>
</ref>
<ref id="B16">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Liu</surname> <given-names>Y. D.</given-names>
</name>
<name>
<surname>Li</surname> <given-names>M. P.</given-names>
</name>
<name>
<surname>Hu</surname> <given-names>J.</given-names>
</name>
<name>
<surname>Xu</surname> <given-names>Z.</given-names>
</name>
<name>
<surname>Cui</surname> <given-names>H. Z.</given-names>
</name>
</person-group> (<year>2021</year>). <article-title>Ldentification of coffee-bean varieties using terahertz detection 'Technology</article-title>. <source>Laser Optoelectronics Progress.</source> <volume>58</volume>, <fpage>433</fpage>&#x2013;<lpage>439</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.3788/LOP202158.1630002</pub-id>
</citation>
</ref>
<ref id="B17">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Liu</surname> <given-names>C. L.</given-names>
</name>
<name>
<surname>Wang</surname> <given-names>S. M.</given-names>
</name>
<name>
<surname>Wu</surname> <given-names>J. Z.</given-names>
</name>
<name>
<surname>Sun</surname> <given-names>X. R.</given-names>
</name>
</person-group> (<year>2020</year>). <article-title>Study on internal quality nondestructive detection of sunflower seed based on terahertz time-domain transmission imaging technology</article-title>. <source>Spectrosc. Spectral Anal.</source> <volume>40</volume> (<issue>11</issue>), <fpage>3384</fpage>&#x2013;<lpage>3389</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.3964/j.issn.1000-0593(2020)11-3384-06</pub-id>
</citation>
</ref>
<ref id="B18">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Liu</surname> <given-names>G. H.</given-names>
</name>
<name>
<surname>Xia</surname> <given-names>R. S.</given-names>
</name>
<name>
<surname>Jiang</surname> <given-names>H.</given-names>
</name>
<name>
<surname>Mei</surname> <given-names>C. L.</given-names>
</name>
<name>
<surname>Huang</surname> <given-names>Y. H.</given-names>
</name>
</person-group> (<year>2014</year>). <article-title>A wavelength selection approach of near infrared spectra based on SCARS strategy and its application</article-title>. <source>Spectrosc. Spectral Analysis.</source> <volume>34</volume>, <fpage>2094</fpage>&#x2013;<lpage>2097</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.3964/j.issn.1000-0593(2014)08-2094-04</pub-id>
</citation>
</ref>
<ref id="B19">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Long</surname> <given-names>Y.</given-names>
</name>
<name>
<surname>Zhao</surname> <given-names>C. J.</given-names>
</name>
<name>
<surname>Li</surname> <given-names>B.</given-names>
</name>
</person-group> (<year>2017</year>). <article-title>The preliminary research on isolated leaf moisture detection using terahertz technology</article-title>. <source>Spectrosc. Spectral Analysis.</source> <volume>37</volume> (<issue>10</issue>), <fpage>3027</fpage>&#x2013;<lpage>3031</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.3964/j.issn.1000-0593(2017)10-3027-05</pub-id>
</citation>
</ref>
<ref id="B20">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Mao</surname> <given-names>H. P.</given-names>
</name>
<name>
<surname>Wang</surname> <given-names>Y. F.</given-names>
</name>
<name>
<surname>Yang</surname> <given-names>N.</given-names>
</name>
<name>
<surname>Liu</surname> <given-names>Y.</given-names>
</name>
<name>
<surname>Zhang</surname> <given-names>X. D.</given-names>
</name>
</person-group> (<year>2022</year>). <article-title>Effects of nutrient solution irrigation quantity and powdery mildew infection on the growth and physiological parameters of greenhouse cucumbers</article-title>. <source>Int. J. Agric. Biol. Engineering.</source> <volume>15</volume> (<issue>2</issue>), <fpage>68</fpage>&#x2013;<lpage>74</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.25165/j.ijabe.20221502.6838</pub-id>
</citation>
</ref>
<ref id="B21">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Ni</surname> <given-names>J. H.</given-names>
</name>
<name>
<surname>Wang</surname> <given-names>Y. Y.</given-names>
</name>
<name>
<surname>Liu</surname> <given-names>Y.</given-names>
</name>
<name>
<surname>Mao</surname> <given-names>H. P.</given-names>
</name>
</person-group> (<year>2021</year>). <article-title>Simulation and validation of photosynthesis of greenhouse tomato based on temporal variation of sucrose yield[J]</article-title>. <source>Trans. Chin. Soc. Agric. Engineering.</source> <volume>7</volume> (<issue>8</issue>), <fpage>223</fpage>&#x2013;<lpage>228</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.11975/j.issn.1002-6819.2021.08.025</pub-id>
</citation>
</ref>
<ref id="B22">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Song</surname> <given-names>X. Z.</given-names>
</name>
<name>
<surname>Huang</surname> <given-names>Y.</given-names>
</name>
<name>
<surname>Yan</surname> <given-names>H.</given-names>
</name>
<name>
<surname>Xiong</surname> <given-names>Y. M.</given-names>
</name>
<name>
<surname>Min</surname> <given-names>S. G.</given-names>
</name>
</person-group> (<year>2016</year>). <article-title>A novel algorithm for spectral interval combination optimization</article-title>. <source>Analytica Chimica Acta</source> <volume>948</volume>, <fpage>19</fpage>&#x2013;<lpage>29</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.1016/j.aca.2016.10.041</pub-id>
</citation>
</ref>
<ref id="B23">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Tian</surname> <given-names>X.</given-names>
</name>
<name>
<surname>Huang</surname> <given-names>W. Q.</given-names>
</name>
<name>
<surname>Li</surname> <given-names>J. B.</given-names>
</name>
<name>
<surname>Fan</surname> <given-names>S. X.</given-names>
</name>
<name>
<surname>Zhang</surname> <given-names>B. H.</given-names>
</name>
</person-group> (<year>2016</year>). <article-title>Measuring the moisture content in maize kernel based on HyperspctralImage of embryo region</article-title>. <source>Spectrosc. Spectral Analysis.</source> <volume>36</volume>, <fpage>3237</fpage>&#x2013;<lpage>3242</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.3964/j.issn.1000-0593(2016)10-3237-06</pub-id>
</citation>
</ref>
<ref id="B24">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Wang</surname> <given-names>Y. F.</given-names>
</name>
<name>
<surname>Mao</surname> <given-names>H. P.</given-names>
</name>
<name>
<surname>Zhang</surname> <given-names>X. D.</given-names>
</name>
<name>
<surname>Liu</surname> <given-names>Y.</given-names>
</name>
<name>
<surname>Du</surname> <given-names>X. X.</given-names>
</name>
</person-group> (<year>2021</year>). <article-title>A rapid detection method for tomato Gray mold spores in greenhouse based on microfluidic chip enrichment and lens-less diffraction image processing</article-title>. <source>Foods</source> <volume>10</volume> (<issue>12</issue>), <elocation-id>3011</elocation-id>. doi:&#xa0;<pub-id pub-id-type="doi">10.3390/foods10123011</pub-id>
</citation>
</ref>
<ref id="B25">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Yada</surname> <given-names>H.</given-names>
</name>
<name>
<surname>Nagai</surname> <given-names>M.</given-names>
</name>
<name>
<surname>Tanaka</surname> <given-names>K.</given-names>
</name>
</person-group> (<year>2008</year>). <article-title>Origin of the fast relaxation component of water and heavy water revealed by terahertz time-domain attenuated total reflection spectroscopy</article-title>. <source>Chem. Phys. Letters.</source> <volume>464</volume>, <fpage>166</fpage>&#x2013;<lpage>170</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.1016/j.cplett.2008.09.015</pub-id>
</citation>
</ref>
<ref id="B26">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Yang</surname> <given-names>Y. L.</given-names>
</name>
<name>
<surname>Zhou</surname> <given-names>S. L.</given-names>
</name>
<name>
<surname>Song</surname> <given-names>J.</given-names>
</name>
<name>
<surname>Huang</surname> <given-names>J.</given-names>
</name>
<name>
<surname>Li</surname> <given-names>G. L.</given-names>
</name>
<name>
<surname>Zhu</surname> <given-names>S. P.</given-names>
</name>
</person-group> (<year>2018</year>). <article-title>Feasibility of terahertz spectroscopy for hybrid purity verification of rice seeds</article-title>. <source>Int. J. Agric. Biol. Engineering.</source> <volume>11</volume>, <fpage>65</fpage>&#x2013;<lpage>69</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.25165/j.ijabe.20181105.3898</pub-id>
</citation>
</ref>
<ref id="B27">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Zhang</surname> <given-names>Z. T.</given-names>
</name>
<name>
<surname>Bian</surname> <given-names>J.</given-names>
</name>
<name>
<surname>Han</surname> <given-names>W. T.</given-names>
</name>
<name>
<surname>Fu</surname> <given-names>Q. P.</given-names>
</name>
<name>
<surname>Chen</surname> <given-names>S. B.</given-names>
</name>
<name>
<surname>Cui</surname> <given-names>T.</given-names>
</name>
</person-group> (<year>2018</year>). <article-title>Cotton moisture stress diagnosis based on canopy temperature characteristics calculated from UAV thermal infrared image</article-title>. <source>Trans. Chin. Soc. Agric. Engineering.</source> <volume>34</volume>, <fpage>77</fpage>&#x2013;<lpage>84</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.11975/j.issn.1002-6819.2018.15.010</pub-id>
</citation>
</ref>
<ref id="B28">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Zhang</surname> <given-names>X. D.</given-names>
</name>
<name>
<surname>Duan</surname> <given-names>C. H.</given-names>
</name>
<name>
<surname>Mao</surname> <given-names>H. P.</given-names>
</name>
<name>
<surname>Gao</surname> <given-names>H. Y.</given-names>
</name>
<name>
<surname>Shi</surname> <given-names>Q.</given-names>
</name>
<name>
<surname>Wang</surname> <given-names>Y. F.</given-names>
</name>
<etal/>
</person-group>. (<year>2021</year>). <article-title>Tomato water stress state detection model by using terahertz spectroscopy technology</article-title>. <source>Trans. Chin. Soc. Agric. Eng.</source> <volume>37</volume> (<issue>15</issue>), <fpage>121</fpage>&#x2013;<lpage>128</lpage>. doi:&#xa0;<pub-id pub-id-type="doi">10.11975/j.issn.1002-6819.2021.15.015</pub-id>
</citation>
</ref>
<ref id="B29">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Zhang</surname> <given-names>X. D.</given-names>
</name>
<name>
<surname>Wang</surname> <given-names>P.</given-names>
</name>
<name>
<surname>Wang</surname> <given-names>Y. F.</given-names>
</name>
<name>
<surname>Hu</surname> <given-names>L.</given-names>
</name>
<name>
<surname>Luo</surname> <given-names>X. W.</given-names>
</name>
<name>
<surname>Mao</surname> <given-names>H. P.</given-names>
</name>
<etal/>
</person-group>. (<year>2022</year>). <article-title>Cucumber powdery mildew detection method based on hyperspectra-terahertz</article-title>. <source>Front. Plant science.</source> <volume>13</volume>. doi:&#xa0;<pub-id pub-id-type="doi">10.3389/fpls.2022.1035731</pub-id>
</citation>
</ref>
<ref id="B30">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Zhao</surname> <given-names>X. T.</given-names>
</name>
<name>
<surname>Zhang</surname> <given-names>S. J.</given-names>
</name>
<name>
<surname>Li</surname> <given-names>B.</given-names>
</name>
<name>
<surname>Li</surname> <given-names>Y. K.</given-names>
</name>
</person-group> (<year>2018</year>). <article-title>Study on moisture content of soybean canopy leaves under DroughtStress using terahertz technology</article-title>. <source>Spectrosc. Spectral Analysis.</source> <volume>38</volume>, <fpage>2350</fpage>&#x2013;<lpage>2354</lpage>
</citation>
</ref>
</ref-list>
</back>
</article>
