<?xml version="1.0" encoding="UTF-8"?><article xml:lang="en" article-type="research-article"><front><journal-meta><journal-id journal-id-type="pmc-domain-id">2909</journal-id><journal-id journal-id-type="pmc-domain">plants</journal-id><journal-title-group><journal-title>Plants</journal-title><abbrev-journal-title>Plants (Basel)</abbrev-journal-title></journal-title-group><publisher><publisher-name>Multidisciplinary Digital Publishing Institute (MDPI)</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="pmcid">PMC12073621</article-id><article-id pub-id-type="pmcaid">12073621</article-id><article-id pub-id-type="pmcaiid">12073621</article-id><article-id pub-id-type="pmid">40364374</article-id><article-id pub-id-type="doi">10.3390/plants14091345</article-id><title-group><article-title>Re-Expression of the Lorenz Asymmetry Coefficient on the Rotated and Right-Shifted Lorenz Curve of Leaf Area Distributions</article-title></title-group><contrib-group content-type="author"><contrib><name name-style="western"><surname>Chen</surname><given-names initials="Y">Yongxia</given-names></name><role>Formal analysis, Writing – original draft</role><xref ref-type="aff" rid="af1-plants-14-01345">1</xref></contrib><contrib><name name-style="western"><surname>Jiang</surname><given-names initials="F">Feixue</given-names></name><role>Investigation</role><xref ref-type="aff" rid="af1-plants-14-01345">1</xref></contrib><contrib><name name-style="western"><surname>Damgaard</surname><given-names initials="CF">Christian Frølund</given-names></name><role>Methodology, Writing – review &amp; editing</role><xref ref-type="aff" rid="af2-plants-14-01345">2</xref><xref rid="c1-plants-14-01345" ref-type="author-notes">*</xref></contrib><contrib><name name-style="western"><surname>Shi</surname><given-names initials="P">Peijian</given-names></name><role>Methodology, Formal analysis, Writing – original draft</role><xref ref-type="aff" rid="af1-plants-14-01345">1</xref><xref rid="c1-plants-14-01345" ref-type="author-notes">*</xref></contrib><contrib><name name-style="western"><surname>Weiner</surname><given-names initials="J">Jacob</given-names></name><role>Methodology, Writing – review &amp; editing, Supervision</role><xref ref-type="aff" rid="af3-plants-14-01345">3</xref></contrib></contrib-group><contrib-group content-type="editor"><contrib><name name-style="western"><surname>Umehara</surname><given-names initials="M">Mikihisa</given-names></name><role>Academic Editor</role></contrib></contrib-group><aff id="af1-plants-14-01345"><label>1</label>Co-Innovation Center for Sustainable Forestry in Southern China, Bamboo Research Institute, College of Civil Engineering, Nanjing Forestry University, Nanjing 210037, China; yongxia@njfu.edu.cn (Y.C.); fxjiang@njfu.edu.cn (F.J.)</aff><aff id="af2-plants-14-01345"><label>2</label>Department of Ecoscience Terrestrial Ecology, Aarhus University, 8000 Aarhus, Denmark</aff><aff id="af3-plants-14-01345"><label>3</label>Department of Plant and Environmental Sciences, University of Copenhagen, Thorvaldsensvej 40, 1871 Frederiksberg, Denmark; jw@plen.ku.dk</aff><author-notes><fn id="c1-plants-14-01345"><label>*</label><p>Correspondence: <email>cfd@ecos.au.dk</email> (C.F.D.); <email>pjshi@njfu.edu.cn</email> (P.S.)</p></fn></author-notes><pub-date><day>29</day><month>4</month><year>2025</year></pub-date><volume>14</volume><issue>9</issue><fpage>1345</fpage><page-range>1345</page-range><pub-history><event event-type="pmc-release"><date><day>14</day><month>5</month><year>2025</year></date></event></pub-history><permissions><copyright-statement>© 2025 by the authors.</copyright-statement><license><license-p>Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (<ext-link xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="https://creativecommons.org/licenses/by/4.0/" ext-link-type="uri">https://creativecommons.org/licenses/by/4.0/</ext-link>).</license-p></license></permissions><self-uri xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="plants-14-01345.pdf" content-type="pmc-pdf"><?cloudpmc-path 0d8d/12073621/1b2f71a13fdd/plants-14-01345.pdf?><?cloudpmc-bucket app?><?size 2187109?></self-uri><abstract id="abstract1"><title>Abstract</title><p>The Gini coefficient, while widely used to quantify inequality in biological size distributions, lacks the capacity to resolve directional asymmetry inherent in Lorenz curves, a critical limitation for understanding skewed resource allocation strategies. To address this, we extend our prior geometric framework of the rotated and right-shifted Lorenz curve (RRLC) by introducing two original asymmetry metrics: the positional shift ratio (<italic>P<sub>L</sub></italic>, defined as <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm1" overflow="scroll"><mml:mrow><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mrow></mml:mrow></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm3" overflow="scroll"><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:math></inline-formula> is the <italic>x</italic>-coordinate of the RRLC’s maximum value point) and the area ratio (<italic>P<sub>A</sub></italic>, defined as <italic>A<sub>L</sub></italic>/(<italic>A<sub>L</sub></italic> + <italic>A<sub>R</sub></italic>), where <italic>A<sub>L</sub></italic> and <italic>A<sub>R</sub></italic> denote the areas under the left and right segments of the RRLC). These indices uniquely dissect contributions of dominant versus small individuals to overall inequality, with <italic>P<sub>L</sub></italic> reflecting the peak position of the RRLC and <italic>P<sub>A</sub></italic> quantifying the area dominance of its left segment. Theoretically, <italic>P<sub>L</sub></italic> directly links to the classical Lorenz asymmetry coefficient <italic>S</italic> (defined as <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm2" overflow="scroll"><mml:mrow><mml:mrow><mml:mi>S</mml:mi><mml:mo>=</mml:mo><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm4" overflow="scroll"><mml:mrow><mml:mrow><mml:mfenced separators="|"><mml:mrow><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:mrow></mml:math></inline-formula> is the tangent point on the original Lorenz curve with a 45° slope) through <italic>S</italic> = 2 − 2<italic>P<sub>L</sub></italic>, bridging geometric transformation and parametric asymmetry analysis. Applied to 480 <italic>Shibataea chinensis</italic> Nakai shoots, our analysis revealed that over 99% exhibited pronounced left-skewed distributions, where abundant large leaves drove the majority of leaf area inequality, challenging assumptions of symmetry in plant canopy resource allocation. The framework’s robustness was further validated by the strong correlation between <italic>P<sub>A</sub></italic> and <italic>P<sub>L</sub></italic>. By transforming abstract Lorenz curves into interpretable bell-shaped performance curves, this work provides a novel toolkit for analyzing asymmetric size distributions in ecology. The proposed metrics can be applied to refine light-use models, monitor phenotypic plasticity under environmental stress, and scale trait variations across biological hierarchies, thereby advancing both theoretical and applied research in plant ecology.</p><sec id="kwd-group1" sec-type="kwd-group" disp-level="2"><p><bold>Keywords:</bold> asymmetry measures, leaf area distributions, Lorenz curve, performance equation, <italic>Shibataea chinensis</italic> Nakai</p></sec></abstract><custom-meta-group><custom-meta><meta-name>status</meta-name><meta-value>released</meta-value></custom-meta><custom-meta><meta-name>display-pdf</meta-name><meta-value>yes</meta-value></custom-meta><custom-meta><meta-name>is-olf</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>is-manuscript</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>is-preprint</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>is-journal-matter</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>is-scanned</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>is-retracted</meta-name><meta-value>no</meta-value></custom-meta></custom-meta-group></article-meta><notes notes-type="article-notes"><sec id="historyarticle-meta1" sec-type="history" disp-level="2"><p>Received 2025 Apr 4; Revised 2025 Apr 26; Accepted 2025 Apr 28; Collection date 2025 May.</p></sec></notes></front><body><sec id="sec1-plants-14-01345" disp-level="1"><title>1. Introduction</title><p>Plant leaves are the primary sites of photosynthesis, serving as the biochemical factories that convert light energy, carbon dioxide, and water into organic compounds essential for growth and survival. As the principal interface between plants and their environment, leaves exhibit remarkable plasticity in morphology and physiology, enabling adaptation to heterogeneous light conditions, which is a critical factor influencing photosynthetic efficiency and plant fitness [<xref rid="B1-plants-14-01345" ref-type="bibr">1</xref>,<xref rid="B2-plants-14-01345" ref-type="bibr">2</xref>]. Given their central role in carbon assimilation, understanding leaf traits and their spatial distribution within plants is important in deciphering ecological strategies and resource utilization. In broad-leaved plants, variation in leaf area allocation across individual shoots or entire canopies reflects adaptive responses to light heterogeneity [<xref rid="B3-plants-14-01345" ref-type="bibr">3</xref>,<xref rid="B4-plants-14-01345" ref-type="bibr">4</xref>]. A well-documented phenomenon is the differentiation between sun and shade leaves. Sun leaves, typically exposed to high irradiance, are characterized by smaller areas, thicker laminas, higher stomatal density, and greater photosynthetic capacity per unit area. These traits enhance water-use efficiency and reduce photodamage under intense light. In contrast, shade leaves, situated in dimmer understory or lower canopy layers, exhibit larger areas, thinner tissues, and lower mass per unit area, maximizing light capture in low-light environments [<xref rid="B5-plants-14-01345" ref-type="bibr">5</xref>,<xref rid="B6-plants-14-01345" ref-type="bibr">6</xref>,<xref rid="B7-plants-14-01345" ref-type="bibr">7</xref>,<xref rid="B8-plants-14-01345" ref-type="bibr">8</xref>]. This intra-canopy plasticity in leaf morphology enables plants to optimize light interception across vertical gradients. For instance, in tree crowns, upper canopy leaves prioritize high-light adaptation, while lower leaves prioritize shade tolerance, thereby collectively enhancing whole-plant carbon gain [<xref rid="B9-plants-14-01345" ref-type="bibr">9</xref>]. Similarly, within a single shoot, leaf area distribution often follows a basipetal gradient, with younger apical leaves smaller and thicker and older basal leaves larger and thinner, aligning with age-dependent light exposure [<xref rid="B10-plants-14-01345" ref-type="bibr">10</xref>,<xref rid="B11-plants-14-01345" ref-type="bibr">11</xref>]. Such patterns suggest that plants strategically allocate leaf area to balance energy investment with photosynthetic returns under spatially variable light. These adaptations are further modulated by species-specific trade-offs between growth rate and stress tolerance, as seen in the contrasting strategies of pioneer versus shade-tolerant species [<xref rid="B12-plants-14-01345" ref-type="bibr">12</xref>]. Collectively, these studies underscore that leaf area distribution within shoots or individuals is not merely a passive outcome of development but a dynamic process driven by selective pressures to maximize light utilization efficiency. In this context it is useful to have a practical method to quantify the inequality of leaf area distributions per shoot or per plant and examine which leaves have contributed to the inequality. This is helpful to account for the strategies for optimizing the use of light by plants.</p><p>The Lorenz curve was originally developed to evaluate inequality in income distributions by plotting the cumulative percentage of the sorted household income in ascending order (<italic>y</italic>′) against the cumulative percentage of the number of households in an economy (<italic>x</italic>′) (<xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>A,C) [<xref rid="B13-plants-14-01345" ref-type="bibr">13</xref>,<xref rid="B14-plants-14-01345" ref-type="bibr">14</xref>,<xref rid="B15-plants-14-01345" ref-type="bibr">15</xref>]. The Gini coefficient [<xref rid="B16-plants-14-01345" ref-type="bibr">16</xref>], which is a measure of inequality, is defined as the proportion of the area formed by the Lorenz curve and the line of absolute equality (i.e., the line segment from (0, 0) to (1, 1)) to the area formed by the line of absolute equality and the two coordinate axes (<xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>A,C). The Lorenz curve and the Gini coefficient have also been used to measure the inequality of biological size distributions [<xref rid="B17-plants-14-01345" ref-type="bibr">17</xref>], such as the distributions of fruit volumes in a vine, leaf areas in a shoot, stomatal areas in a micrograph, petal areas in a flower, and tree diameters at breast height in a quadrat [<xref rid="B18-plants-14-01345" ref-type="bibr">18</xref>]. The Gini coefficient is a summary statistic that does not capture all the information present in the Lorenz curve [<xref rid="B19-plants-14-01345" ref-type="bibr">19</xref>]. Furthermore, multiple distinct Lorenz curves can share the same Gini coefficient. The Lorenz curve reveals three size distribution patterns: (i) inequality driven by abundant large individuals, (ii) inequality dominated by a few large individuals, and (iii) parity in contributions between small and large individuals. If the Lorenz curve is a continuous function, there is a point on the Lorenz curve (denoted as <bold>the point of tangency</bold>, i.e., <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm5" overflow="scroll"><mml:mrow><mml:mrow><mml:mfenced separators="|"><mml:mrow><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:mrow></mml:math></inline-formula> in <xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>A,C) where the derivative equals tan(π/4), i.e., the tangent of the Lorenz curve at this point is parallel to the egalitarian line. For pattern (i), the point of tangency is located in the lower left area relative to the straight line through (1, 0) and (0, 1), denoted as <bold>the axis of symmetry</bold> (<xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>A); for pattern (ii), the point of tangency is located in the upper right area relative to the axis of symmetry (<xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>C); for pattern (iii), the point of tangency is exactly the intersection point between the Lorenz curve and the axis of symmetry. It is apparent that pattern (iii) signifies a symmetrical Lorenz curve about the axis of symmetry.</p><fig id="plants-14-01345-f001" position="float"><?disp-level 2?><label>Figure 1</label><caption><p>The Lorenz curves (<bold>A</bold>,<bold>C</bold>) and their rotated and right-shifted forms (<bold>B</bold>,<bold>D</bold>). <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm48" overflow="scroll"><mml:mrow><mml:mrow><mml:mfenced separators="|"><mml:mrow><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:mrow></mml:math></inline-formula> (the blue open circle) in panels (<bold>A</bold>,<bold>C</bold>) is the point of tangency at which the tangent of the Lorenz curve is parallel to the egalitarian line through the points (0, 0) and (1, 1). The dashed line through the two points (0, 1) and (1, 0) is defined as the axis of symmetry. Panels (<bold>B</bold>,<bold>D</bold>) exhibit the rotated and right-shifted Lorenz curves, which can be described by the performance equation. <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm6" overflow="scroll"><mml:mrow><mml:mrow><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mo> </mml:mo><mml:msub><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mrow></mml:math></inline-formula> is the maximum value point of the performance curve, which is obtained by rotating <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm7" overflow="scroll"><mml:mrow><mml:mrow><mml:mfenced separators="|"><mml:mrow><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:mrow></mml:math></inline-formula> counterclockwise by 3/4π and shifting it to the right by <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm8" overflow="scroll"><mml:mrow><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mrow></mml:math></inline-formula>. In panels (<bold>B</bold>,<bold>D</bold>), <italic>A<sub>L</sub></italic> represents the area of the region formed by the performance’s left part and the <italic>x</italic>-axis, and <italic>A<sub>R</sub></italic> represents the area of the region formed by the performance’s right part and the <italic>x</italic>-axis.</p></caption><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" content-type="image" xlink:href="plants-14-01345-g001.jpg"><?cloudpmc-path blobs/0d8d/12073621/f49c6c8d00bb/plants-14-01345-g001.jpg?><?cloudpmc-bucket cdn?><?image-server-status LOAD_COMPLETED?><?original-height 3216?><?original-width 3164?><?scaled-height 804?><?scaled-width 791?></graphic><graphic xmlns:xlink="http://www.w3.org/1999/xlink" content-type="thumb" xlink:href="plants-14-01345-g001.gif"><?cloudpmc-path blobs/0d8d/12073621/f5e2205f0f32/plants-14-01345-g001.gif?><?cloudpmc-bucket cdn?></graphic></alternatives></fig><p>Let <italic>x</italic>′ represent the cumulative percentage of the number of individuals in a statistical unit (e.g., the percentage of the number of fruits in a vine, that of stomata in a micrograph, that of leaves in a shoot, that of tree diameters at breast height in a quadrat), and <italic>y</italic>′ represent the cumulative percentage of size, i.e., the horizontal and vertical coordinates of the Lorenz curve (<xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>A,C). Let <italic>x</italic>′ + <italic>y</italic>′ = <italic>C</italic> <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm9" overflow="scroll"><mml:mrow><mml:mrow><mml:mo>⟺</mml:mo></mml:mrow></mml:mrow></mml:math></inline-formula> <italic>y</italic>′ = −<italic>x</italic>′ + <italic>C</italic>, where <italic>C</italic> is a constant between 0 and <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm10" overflow="scroll"><mml:mrow><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mrow></mml:math></inline-formula>. The equation can generate a group of <italic>y</italic>′ vs. <italic>x</italic>′ straight lines with the same slope being equal to negative unity in the <italic>x</italic>′−<italic>y</italic>′ plane. Let <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm11" overflow="scroll"><mml:mrow><mml:mrow><mml:mi>S</mml:mi><mml:mo>=</mml:mo><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm12" overflow="scroll"><mml:mrow><mml:mrow><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm13" overflow="scroll"><mml:mrow><mml:mrow><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mrow></mml:math></inline-formula> are the horizontal and vertical coordinates of the point of tangency [<xref rid="B19-plants-14-01345" ref-type="bibr">19</xref>]. It is apparent that <italic>S</italic> &lt; 1 indicates pattern (i) for overall inequality; <italic>S</italic> &gt; 1 indicates pattern (ii) for overall inequality; <italic>S</italic> = 1 indicates pattern (iii). Our prior study shows that after the Lorenz curve of biological size distributions is rotated counterclockwise by 3/4π and then shifted to the right by <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm14" overflow="scroll"><mml:mrow><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mrow></mml:math></inline-formula>, it becomes a skewed or symmetrical bell-shaped curve (<xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>B,D) that can be well described by a nonlinear equation called the performance equation [<xref rid="B11-plants-14-01345" ref-type="bibr">11</xref>,<xref rid="B18-plants-14-01345" ref-type="bibr">18</xref>]. The performance equation was first proposed to describe the effect of body temperature (<italic>x</italic>) on the jumping distance (<italic>y</italic>) of green frogs [<xref rid="B20-plants-14-01345" ref-type="bibr">20</xref>], which has its original form written as follows:</p><disp-formula id="FD1-plants-14-01345"><label>(1)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm15" display="block" overflow="scroll"><mml:mrow><mml:mrow><mml:mi>y</mml:mi><mml:mo>=</mml:mo><mml:mi>c</mml:mi><mml:mfenced><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>−</mml:mo><mml:msub><mml:mi>K</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mfenced><mml:mrow><mml:mi>x</mml:mi><mml:mo>−</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn>1</mml:mn></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:msup></mml:mrow></mml:mfenced><mml:mfenced><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo>−</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula><p>
where <italic>c</italic>, <italic>K</italic><sub>1</sub>, <italic>K</italic><sub>2</sub>, <italic>x</italic><sub>1</sub>, and <italic>x</italic><sub>2</sub> are the parameters that can be estimated by minimizing a target function, e.g., the residual sum of squares (RSS) between the observed and predicted <italic>y</italic> values, using the nonlinear least-squares method [<xref rid="B21-plants-14-01345" ref-type="bibr">21</xref>,<xref rid="B22-plants-14-01345" ref-type="bibr">22</xref>,<xref rid="B23-plants-14-01345" ref-type="bibr">23</xref>]. In the present study, <italic>x</italic> and <italic>y</italic> represent the horizontal and vertical coordinates the rotated and right-shifted Lorenz curve (denoted as RRLC) to replace their original meanings of body temperature and jumping distance; the original temperature axis (i.e., the <italic>x</italic>-axis) then represents the rotated and right-shifted egalitarian line, and <italic>x</italic><sub>1</sub> and <italic>x</italic><sub>2</sub> exactly correspond to its two endpoints, i.e., (0, 0) and (<inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm16" overflow="scroll"><mml:mrow><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mrow></mml:math></inline-formula>, 0) (<xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>B,D). Thus, Equation (1) can be simplified to the following form [<xref rid="B11-plants-14-01345" ref-type="bibr">11</xref>]:</p><disp-formula id="FD2-plants-14-01345"><label>(2)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm17" display="block" overflow="scroll"><mml:mrow><mml:mrow><mml:mi>y</mml:mi><mml:mo>=</mml:mo><mml:mi>c</mml:mi><mml:mfenced><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>−</mml:mo><mml:msub><mml:mi>K</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mi>x</mml:mi></mml:mrow></mml:msup></mml:mrow></mml:mfenced><mml:mfenced><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo>−</mml:mo><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:mfenced><mml:mo>.</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula><p> Here, <italic>c</italic> is a scaling parameter influencing the maximum value of the performance curve (i.e., the curve generated by the performance equation representing the RRLC); <italic>K</italic><sub>1</sub> and <italic>K</italic><sub>2</sub> determine the curvature of the performance curve’s left part and that of the performance curve’s right part about the vertical line through the maximum value point on the performance curve. Since <italic>x</italic><sub>1</sub> and <italic>x</italic><sub>2</sub> are predefined model parameters (i.e., the endpoints of the RRLC) in Equation (1), only the parameters <italic>c</italic>, <italic>K</italic><sub>1</sub>, and <italic>K</italic><sub>2</sub> in Equation (2) require estimation once experimental data are available. When <italic>K</italic><sub>1</sub> is equal to <italic>K</italic><sub>2</sub>, the performance curve is bilaterally symmetrical about <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm18" overflow="scroll"><mml:mrow><mml:mrow><mml:mi>x</mml:mi><mml:mo>=</mml:mo><mml:mrow><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow><mml:mo>/</mml:mo><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:mrow></mml:mrow></mml:mrow></mml:math></inline-formula>. And the point of tangency in the <italic>x</italic>′-<italic>y</italic>′ plane corresponds to the maximum point on the RRLC in the <italic>x</italic>–<italic>y</italic> plane (<xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>). To increase the flexibility of data fitting of the performance equation, ref. [<xref rid="B11-plants-14-01345" ref-type="bibr">11</xref>] also proposed a generalized version of the performance equation, written as follows:</p><disp-formula id="FD3-plants-14-01345"><label>(3)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm19" display="block" overflow="scroll"><mml:mrow><mml:mrow><mml:mi>y</mml:mi><mml:mo>=</mml:mo><mml:mi>c</mml:mi><mml:msup><mml:mrow><mml:mfenced><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>−</mml:mo><mml:msub><mml:mi>K</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mi>x</mml:mi></mml:mrow></mml:msup></mml:mrow></mml:mfenced></mml:mrow><mml:mi>a</mml:mi></mml:msup><mml:msup><mml:mrow><mml:mfenced><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:mo stretchy="false">(</mml:mo><mml:mi>x</mml:mi><mml:mo>−</mml:mo><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:mfenced></mml:mrow><mml:mi>b</mml:mi></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula><p>
where <italic>a</italic> and <italic>b</italic> are two additional parameters that also can be estimated by minimizing the RSS between the observed and predicted <italic>y</italic> values using the nonlinear least-squares method [<xref rid="B21-plants-14-01345" ref-type="bibr">21</xref>,<xref rid="B22-plants-14-01345" ref-type="bibr">22</xref>,<xref rid="B23-plants-14-01345" ref-type="bibr">23</xref>]. The performance equation and its generalized version were validated to fit the rotated and right-shifted observations of <italic>y</italic>′ vs. <italic>x</italic>′ in biological size distributions regardless of the size distribution function [<xref rid="B18-plants-14-01345" ref-type="bibr">18</xref>,<xref rid="B24-plants-14-01345" ref-type="bibr">24</xref>].</p><p>It is easy to determine whether the Lorenz curve is asymmetrical or symmetrical by observing the shape of the performance curve in the <italic>x–y</italic> plane. Let <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm20" overflow="scroll"><mml:mrow><mml:mrow><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mo> </mml:mo><mml:msub><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mrow></mml:math></inline-formula> represent the rotated and right-shifted point of tangency, which is the maximum value point on the RRLC (<xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>B,D). To determine the degree of asymmetry of the RRLC, we only need to examine the numerical value of <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm21" overflow="scroll"><mml:mrow><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mrow></mml:mrow></mml:mrow></mml:math></inline-formula> (denoted as <italic>P<sub>L</sub></italic>) or the proportion of the area of the region formed the left part of the performance curve and the <italic>x</italic>-axis to the whole area of the region formed by the performance curve and the <italic>x</italic>-axis (denoted as <italic>P<sub>A</sub></italic>). If <italic>P<sub>L</sub></italic> &gt; 0.5 or <italic>P<sub>A</sub></italic> &gt; 0.5, the RRLC is left-skewed; if <italic>P<sub>L</sub></italic> &lt; 0.5 or <italic>P<sub>A</sub></italic> &lt; 0.5, the RRLC is right-skewed; if <italic>P<sub>L</sub></italic> = 0.5 or <italic>P<sub>A</sub></italic> = 0.5, the RRLC is bilaterally symmetrical about the vertical line <italic>x</italic> = <italic>x<sub>c</sub></italic>. In the present study, we examined the relationships among the two asymmetry measures for the RRLC in the <italic>x</italic>–<italic>y</italic> plane here and the Lorenz asymmetry coefficient (<italic>S</italic>) in the <italic>x</italic>′<italic>-y</italic>′ plane using 480 shoots of <italic>Shibataea chinensis</italic> Nakai, an herbaceous bamboo species. This work can provide a useful tool for detecting the contribution of the largest leaves to the inequality of leaf area distribution per shoot or per individual plant.</p><p>While the Gini coefficient has been widely adopted to quantify inequality in biological size distributions, its inherent limitation in capturing the directional asymmetry of Lorenz curves necessitates novel analytical frameworks. In this study, we introduce the RRLC coupled with two redefined asymmetry metrics (i.e., <italic>P<sub>L</sub></italic> and <italic>P<sub>A</sub></italic>). This is a methodological advancement that uniquely disentangles the contributions of dominant large individuals from cumulative small-individual effects. Unlike conventional approaches that rely solely on the Lorenz asymmetry coefficient (<italic>S</italic>), our RRLC-based metrics leverage geometric transformations and performance equation parameterization to provide dual perspectives on distributional skewness: <italic>P<sub>L</sub></italic> quantifies positional shifts of the RRLC peak, while <italic>P<sub>A</sub></italic> integrates area ratios between left and right segments of the performance curve. This dual-metric system addresses a critical gap in ecological inequality analysis by enabling multidimensional characterization of resource allocation strategies, particularly in light-limited environments where large leaves disproportionately drive photosynthetic efficiency. Beyond plant ecology, our framework offers a generalizable tool for analyzing asymmetric size distributions in fields ranging from canopy physiology to biodiversity conservation, where disentangling outlier-driven inequality is essential for mechanistic modeling.</p></sec><sec id="sec2-plants-14-01345" disp-level="1"><title>2. Materials and Methods</title><sec id="sec2dot1-plants-14-01345" disp-level="2"><title>2.1. Leaf Sampling</title><p>We randomly sampled 480 <italic>S. chinensis</italic> shoots growing in the Nanjing Forestry University Xinzhuang campus (118°48′53″ E, 32°4′52″ N) in the autumn of 2023. The number of leaves per shoot ranges from 8 to 40. The shoots were cut at the ground, then wrapped with wet paper, and taken back to the lab within one hour. All leaves were sampled from each of the 480 shoots, and the pseudo-petioles of leaves were removed.</p></sec><sec id="sec2dot2-plants-14-01345" disp-level="2"><title>2.2. Data Acquisition</title><p>All leaves on the 240 shoots were scanned at a 1:1 scale to .jpg images with a photo scanner (V550, Epson Indonesia, Batam, Indonesia) at a resolution of 600 dpi and then transformed into black-and-white .bmp images using Adobe Photoshop (version 9.0; Adobe, San Jose, CA, USA). An M-file in Matlab (version ≥ 2009a; MathWorks, Natick, MA, USA) presented in [<xref rid="B25-plants-14-01345" ref-type="bibr">25</xref>,<xref rid="B26-plants-14-01345" ref-type="bibr">26</xref>] was used to extract leaf boundary coordinates in the .bmp images. The 240 shoots comprised 4638 leaves in total, with each leaf containing 4809 ± 865 boundary points (mean ± SD) extracted from digitized images. To balance computational efficiency with geometric fidelity, a uniform subsample of 2000 boundary points for each leaf was selected to calculate the leaf area (<italic>A</italic>) using the “bilat” function in the “biogeom” package (v1.3.5) [<xref rid="B27-plants-14-01345" ref-type="bibr">27</xref>] implemented in R statistical software (v4.2.0) [<xref rid="B28-plants-14-01345" ref-type="bibr">28</xref>]. Here, the “bilat” function calculates polygon area by first identifying adjacent boundary points through minimum Euclidean distance analysis and then applying the shoelace formula to the ordered coordinate sequence, thereby reconstructing closed contours for precise areal computation. Due to the excessive scanning workload, we did not directly scan the leaves for the other 240 shoots to determine their <italic>A</italic> values. For all leaves of the other 240 shoots (5455 leaves in total), we measured the length and width of each leaf and calculated individual <italic>A</italic> using the Montgomery equation that assumes <italic>A</italic> to be proportional to the product of leaf length (<italic>L</italic>) and width (<italic>W</italic>) [<xref rid="B29-plants-14-01345" ref-type="bibr">29</xref>,<xref rid="B30-plants-14-01345" ref-type="bibr">30</xref>]:</p><disp-formula id="FD4-plants-14-01345"><label>(4)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm22" display="block" overflow="scroll"><mml:mrow><mml:mrow><mml:mi>A</mml:mi><mml:mo>=</mml:mo><mml:mi>k</mml:mi><mml:mi>L</mml:mi><mml:mi>W</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula><p>
where <italic>k</italic> is the proportionality coefficient to be estimated. It is equal to two-thirds, which was validated using the 240 individual leaves of this bamboo species [<xref rid="B31-plants-14-01345" ref-type="bibr">31</xref>].</p><p>The raw data of leaf area of the 240 <italic>S. chinensis</italic> shoots, and the raw data of leaf length and width of the other 240 <italic>S. chinensis</italic> shoots are accessible from the online Supplementary Tables S1 and S3 in [<xref rid="B31-plants-14-01345" ref-type="bibr">31</xref>].</p></sec><sec id="sec2dot3-plants-14-01345" disp-level="2"><title>2.3. Three Indicators for Measuring the Asymmetry of the Lorenz Curve</title><p>We used three measures for quantifying the degree of asymmetry of the Lorenz curve as mentioned above. The asymmetry Lorenz coefficient takes the following form as [<xref rid="B19-plants-14-01345" ref-type="bibr">19</xref>]:</p><disp-formula id="FD5-plants-14-01345"><label>(5)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm23" display="block" overflow="scroll"><mml:mrow><mml:mrow><mml:mi>S</mml:mi><mml:mo>=</mml:mo><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>,</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula><p>
where <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm24" overflow="scroll"><mml:mrow><mml:mrow><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm25" overflow="scroll"><mml:mrow><mml:mrow><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mrow></mml:math></inline-formula> are the horizontal and vertical coordinates of the point of tangency in the <italic>x</italic>′–<italic>y</italic>′ plane (<xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>A,C). When <italic>S</italic> &lt; 1, the RRLC is left-skewed; when <italic>S</italic> &gt; 1, the RRLC is right-skewed; when S = 1, the RRLC is bilaterally symmetrical about the vertical line <italic>x</italic> = <italic>x<sub>c</sub></italic> (<xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>B,D).</p><p>The proportion of the line segment from the point (0, 0) to the point (<italic>x<sub>c</sub></italic>, 0) (i.e., the point on the <italic>x</italic>-axis associated with the maximum value of the performance curve) to <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm26" overflow="scroll"><mml:mrow><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mrow></mml:math></inline-formula> on the RRLC, which is denoted as <italic>P<sub>L</sub></italic>:</p><disp-formula id="FD6-plants-14-01345"><label>(6)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm27" display="block" overflow="scroll"><mml:mrow><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>L</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mrow><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mrow><mml:mo>.</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula><p> When <italic>P<sub>L</sub></italic> &gt; 0.5, the RRLC is left-skewed; when <italic>P<sub>L</sub></italic> &lt; 0.5, the RRLC is right-skewed; when <italic>P<sub>L</sub></italic> = 0.5, the RRLC is bilaterally symmetrical about the vertical line <italic>x</italic> = <italic>x<sub>c</sub></italic>. There is an explicit linear relationship between <italic>S</italic> and <italic>P<sub>L</sub></italic>: <italic>S</italic> = 2 − 2<italic>P<sub>L</sub></italic> (<xref rid="app2-plants-14-01345" ref-type="sec">Appendix A</xref>).</p><p>The proportion of the area of the region formed by the performance curve’s left part (<italic>A<sub>L</sub></italic>) and the <italic>x</italic>-axis to the area of the region formed by the whole performance curve (i.e., the RRLC) and the <italic>x</italic>-axis (i.e., the sum of the left part’s area and the right part’s area (<italic>A<sub>L</sub></italic> + <italic>A<sub>R</sub></italic>); <xref rid="plants-14-01345-f001" ref-type="fig">Figure 1</xref>B,D), which is denoted as <italic>P<sub>A</sub></italic>, written as follows:</p><disp-formula id="FD7-plants-14-01345"><label>(7)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm28" display="block" overflow="scroll"><mml:mrow><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mrow><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>L</mml:mi></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mrow><mml:mfenced><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>L</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>A</mml:mi><mml:mi>R</mml:mi></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mrow><mml:mo>.</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula><p> When <italic>P<sub>A</sub></italic> &gt; 0.5, the RRLC is left-skewed; when <italic>P<sub>A</sub></italic> &lt; 0.5, the RRLC is right-skewed; when <italic>P<sub>A</sub></italic> = 0.5, the RRLC is bilaterally symmetrical about the vertical line <italic>x</italic> = <italic>x<sub>c</sub></italic>. <italic>P<sub>A</sub></italic> is similar to <italic>P<sub>L</sub></italic>. However, <italic>P<sub>A</sub></italic> contains more information, including the maximum value point of the performance curve.</p><p>Because <italic>S</italic> and <italic>P<sub>L</sub></italic> have an explicit linear relationship (<xref rid="app2-plants-14-01345" ref-type="sec">Appendix A</xref>), we used the reduced major axis (RMA) regression [<xref rid="B32-plants-14-01345" ref-type="bibr">32</xref>] to test the probable relationship between <italic>P<sub>L</sub></italic> and <italic>P<sub>A</sub></italic>. The RMA regression estimates the slope to be the square root of the quotient of the variance of the dependent variable and that of the independent variable if the covariance of the dependent and independent variables is positive. If we exchange the dependent and independent variables, the estimated slope is the reciprocal of the estimated slope of the unexchanged dependent and independent variables.</p><p>The first derivation of the performance equation was provided in [<xref rid="B33-plants-14-01345" ref-type="bibr">33</xref>]. However, there is no analytical solution for the maximum value point of the performance curve. We calculated the numerical solution of <italic>x<sub>c</sub></italic> and <italic>y<sub>c</sub></italic> (see below for details).</p></sec><sec id="sec2dot4-plants-14-01345" disp-level="2"><title>2.4. Parametric Estimation of the Performance Equation</title><p>We used Equation (2) to describe the rotated and right-shifted Lorenz curve (RRLC). The parameters of Equation (2) were estimated by minimizing the residual sum of squares (RSS) between the observed and predicted <italic>y</italic> values using the “L-BFGS-B” optimization algorithm [<xref rid="B34-plants-14-01345" ref-type="bibr">34</xref>]. The lower and upper bounds for the three parameters, i.e., <italic>c</italic>, <italic>K</italic><sub>1</sub> and <italic>K</italic><sub>2</sub>, were set to be (0, <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm29" overflow="scroll"><mml:mrow><mml:mrow><mml:mrow><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow><mml:mo>/</mml:mo><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:mrow></mml:mrow></mml:mrow></mml:math></inline-formula>), (0, 50), and (0, 50), respectively, in nonlinear regression. The root-mean-square error (RMSE = <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm30" overflow="scroll"><mml:mrow><mml:mrow><mml:msqrt><mml:mrow><mml:mrow><mml:mi mathvariant="normal">R</mml:mi><mml:mi mathvariant="normal">S</mml:mi><mml:mi mathvariant="normal">S</mml:mi></mml:mrow><mml:mo>/</mml:mo><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:mrow></mml:msqrt></mml:mrow></mml:mrow></mml:math></inline-formula>) is usually used to reflect the goodness of fit of nonlinear regression, where <italic>n</italic> represents the total number of leaves in a shoot. However, given the variation of the maximum value point on the RRLC across shoots, we used an adjusted root-mean-square error (RMSE<sub>adj</sub>), which equals the RMSE divided by the maximum value of the performance curve [<xref rid="B35-plants-14-01345" ref-type="bibr">35</xref>], written as follows:</p><disp-formula id="FD8-plants-14-01345"><label>(8)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm31" display="block" overflow="scroll"><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>RMSE</mml:mi></mml:mrow><mml:mrow><mml:mi>adj</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle scriptlevel="0" displaystyle="true"><mml:mfrac><mml:mrow><mml:msqrt><mml:mrow><mml:mrow><mml:mrow><mml:mi>RSS</mml:mi></mml:mrow><mml:mo>/</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:mrow></mml:msqrt></mml:mrow><mml:mrow><mml:msub><mml:mi>y</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula><p> As a rule of thumb, a &lt; 0.05 RMSE<sub>adj</sub> indicates a good fit.</p></sec><sec id="sec2dot5-plants-14-01345" disp-level="2"><title>2.5. Calculation of the Gini Coefficient for the Leaf Area Distribution per Shoot</title><p>After obtaining the parameters of Equation (2), the Gini coefficient is calculated using the following formula [<xref rid="B11-plants-14-01345" ref-type="bibr">11</xref>]:</p><disp-formula id="FD9-plants-14-01345"><label>(9)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm32" display="block" overflow="scroll"><mml:mrow><mml:mrow><mml:mrow><mml:mi>Gini</mml:mi><mml:mo> </mml:mo><mml:mi>coefficient</mml:mi></mml:mrow><mml:mo>=</mml:mo><mml:mn>2</mml:mn><mml:mo>×</mml:mo><mml:mstyle displaystyle="true"><mml:mrow><mml:msubsup><mml:mo>∫</mml:mo><mml:mn>0</mml:mn><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:msubsup><mml:mrow><mml:mi>y</mml:mi><mml:mfenced><mml:mrow><mml:mi>x</mml:mi><mml:mo>;</mml:mo><mml:mo> </mml:mo><mml:mstyle mathvariant="bold" mathsize="normal"><mml:mover accent="true"><mml:mi>θ</mml:mi><mml:mo>^</mml:mo></mml:mover></mml:mstyle></mml:mrow></mml:mfenced><mml:mi>d</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:mrow></mml:mstyle></mml:mrow></mml:mrow></mml:math></disp-formula><p>
where <italic>y</italic> is given by Equation (2), and <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm33" overflow="scroll"><mml:mrow><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi mathvariant="bold">θ</mml:mi></mml:mrow><mml:mo>^</mml:mo></mml:mover></mml:mrow></mml:mrow></mml:math></inline-formula> represents the parametric vector including the estimates of <italic>c</italic>, <italic>K</italic><sub>1</sub>, and <italic>K</italic><sub>2</sub>.</p><p>The calculations of the above four indices were carried out using the statistical software R (v4.2.0) [<xref rid="B28-plants-14-01345" ref-type="bibr">28</xref>]. The nonlinear regression was formed using the “optim” function.</p></sec></sec><sec id="sec3-plants-14-01345" disp-level="1"><title>3. Results</title><p>The performance equation (i.e., Equation (2)) well fitted the observations, with most shoots (98.1%, i.e., 471 out of the 480 shoots) having &lt; 0.05 RMSE<sub>adj</sub> values (<xref rid="plants-14-01345-f002" ref-type="fig">Figure 2</xref>). <xref rid="plants-14-01345-f003" ref-type="fig">Figure 3</xref> exhibits an example of data fitting for a representative shoot (the 223rd shoot). The first Lorenz asymmetry coefficients (<italic>S</italic>, Equation (5)) ranged from 0.310 to 1.006, with the mean ± standard error 0.710 ± 0.098 (<xref rid="plants-14-01345-f004" ref-type="fig">Figure 4</xref>A). The second Lorenz asymmetry coefficients (<italic>P<sub>L</sub></italic>, Equation (6)) ranged from 0.497 to 0.845, with the mean ± standard error 0.646 ± 0.049 (<xref rid="plants-14-01345-f004" ref-type="fig">Figure 4</xref>B). The third Lorenz asymmetry coefficients (<italic>P<sub>A</sub></italic>, Equation (7)) ranged from 0.498 to 0.830, with the mean ± standard error 0.617 ± 0.044 (<xref rid="plants-14-01345-f004" ref-type="fig">Figure 4</xref>C). The consistent alignment among <italic>S</italic>, <italic>P<sub>L</sub></italic>, and <italic>P<sub>A</sub></italic> metrics demonstrates that abundant larger leaves disproportionately contribute to the inequality in leaf area distribution across the 479 shoots. The Gini coefficients ranged from 0.046 to 0.272, with the mean ± standard error 0.156 ± 0.047 (<xref rid="plants-14-01345-f004" ref-type="fig">Figure 4</xref>D), indicating large variation in the inequality of leaf area distributions among the 480 shoots. There was a robust linear relationship between <italic>P<sub>A</sub></italic> and <italic>P<sub>L</sub></italic> (<italic>r</italic><sup>2</sup> = 0.982; <xref rid="plants-14-01345-f005" ref-type="fig">Figure 5</xref>). The estimates of model parameters, three Lorenz asymmetry measures (i.e., <italic>S</italic>, <italic>P<sub>L</sub></italic>, and <italic>P<sub>A</sub></italic>), and Gini coefficients for the 480 <italic>S</italic>. <italic>chinensis</italic> shoots are available in <xref rid="app1-plants-14-01345" ref-type="sec">Table S1</xref>.</p><fig id="plants-14-01345-f002" position="float"><?disp-level 2?><label>Figure 2</label><caption><p>Box plot of the adjusted root-mean-square errors (Equation (8)) of the performance equation fit to the 480 shoots. Here, the vertical dashed line represents the value of 0.05.</p></caption><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" content-type="image" xlink:href="plants-14-01345-g002.jpg"><?cloudpmc-path blobs/0d8d/12073621/aba07ea843fd/plants-14-01345-g002.jpg?><?cloudpmc-bucket cdn?><?image-server-status LOAD_COMPLETED?><?original-height 1632?><?original-width 1641?><?scaled-height 652?><?scaled-width 656?></graphic><graphic xmlns:xlink="http://www.w3.org/1999/xlink" content-type="thumb" xlink:href="plants-14-01345-g002.gif"><?cloudpmc-path blobs/0d8d/12073621/6fd4abbb67a2/plants-14-01345-g002.gif?><?cloudpmc-bucket cdn?></graphic></alternatives></fig><fig id="plants-14-01345-f003" position="float"><?disp-level 2?><label>Figure 3</label><caption><p>Fitted results for an individual shoot (the 223rd shoot) of <italic>S. chinensis</italic> using the performance equation. Panel (<bold>A</bold>) shows the comparison of the observations and the predicted original Lorenz curve, and the 45° straight line represents the egalitarian line; panel (<bold>B</bold>) shows the comparison of the observations and the predicted Lorenz curve after being rotated and right-shifted. The closed circles represent the observations, and the red curve represents predicted values; the open circle represents the point of tangency in panel (<bold>A</bold>), or the maximum value point of the performance curve in panel (<bold>B</bold>). In panel (<bold>A</bold>), the letters <italic>c</italic>, <italic>K</italic><sub>1,</sub> and <italic>K</italic><sub>2</sub> with hats represent the estimated parameters of the performance equation; RMSE<sub>adj</sub> represents the adjusted root-mean-square error; and <italic>n</italic> represents the number of leaves on the individual shoot. The Gini coefficient is estimated as double the area of the region between the performance curve (i.e., the red curve in panel (<bold>B</bold>)) and the <italic>x</italic>-axis.</p></caption><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" content-type="image" xlink:href="plants-14-01345-g003.jpg"><?cloudpmc-path blobs/0d8d/12073621/537905cd90d7/plants-14-01345-g003.jpg?><?cloudpmc-bucket cdn?><?image-server-status LOAD_COMPLETED?><?original-height 1650?><?original-width 3317?><?scaled-height 367?><?scaled-width 737?></graphic><graphic xmlns:xlink="http://www.w3.org/1999/xlink" content-type="thumb" xlink:href="plants-14-01345-g003.gif"><?cloudpmc-path blobs/0d8d/12073621/e81a46a84d75/plants-14-01345-g003.gif?><?cloudpmc-bucket cdn?></graphic></alternatives></fig><fig id="plants-14-01345-f004" position="float"><?disp-level 2?><label>Figure 4</label><caption><p>Distributions of three asymmetry measures (<italic>S</italic>, <italic>P<sub>L</sub></italic>, and <italic>P<sub>A</sub></italic>) for the Lorenz curves (<bold>A</bold>–<bold>C</bold>), and the Gini coefficients (<bold>D</bold>) for the 480 <italic>S. chinensis</italic> shoots. “Mean” and “Median” represent the mean and median, respectively; CV is the coefficient of variation; and <italic>p</italic> is the probability that the data are consistent with the null hypothesis of a normal distribution.</p></caption><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" content-type="image" xlink:href="plants-14-01345-g004.jpg"><?cloudpmc-path blobs/0d8d/12073621/c5aecade3fe2/plants-14-01345-g004.jpg?><?cloudpmc-bucket cdn?><?image-server-status LOAD_COMPLETED?><?original-height 2630?><?original-width 2637?><?scaled-height 751?><?scaled-width 753?></graphic><graphic xmlns:xlink="http://www.w3.org/1999/xlink" content-type="thumb" xlink:href="plants-14-01345-g004.gif"><?cloudpmc-path blobs/0d8d/12073621/6bccb7f54d8b/plants-14-01345-g004.gif?><?cloudpmc-bucket cdn?></graphic></alternatives></fig><fig id="plants-14-01345-f005" position="float"><?disp-level 2?><label>Figure 5</label><caption><p>Linear fit to the two asymmetry measures (<italic>P<sub>A</sub></italic> versus <italic>P<sub>L</sub></italic>). The open circles represent the observations; CI<sub>intercept</sub> represents the 95% confidence interval of the intercept; CI<sub>slope</sub> represents the 95% confidence interval of the slope; <italic>r</italic><sup>2</sup> is the coefficient of determination of the linear fitting; and <italic>N</italic> is the sample size, i.e., the total number of shoots.</p></caption><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" content-type="image" xlink:href="plants-14-01345-g005.jpg"><?cloudpmc-path blobs/0d8d/12073621/5b3f7cd747d8/plants-14-01345-g005.jpg?><?cloudpmc-bucket cdn?><?image-server-status LOAD_COMPLETED?><?original-height 1593?><?original-width 1640?><?scaled-height 637?><?scaled-width 656?></graphic><graphic xmlns:xlink="http://www.w3.org/1999/xlink" content-type="thumb" xlink:href="plants-14-01345-g005.gif"><?cloudpmc-path blobs/0d8d/12073621/5e73dfbf867a/plants-14-01345-g005.gif?><?cloudpmc-bucket cdn?></graphic></alternatives></fig></sec><sec id="sec4-plants-14-01345" disp-level="1"><title>4. Discussion</title><p>This study re-examined the Lorenz asymmetry coefficient (<italic>S</italic>) through the lens of rotated and right-shifted Lorenz curves (RRLCs), proposing two novel measures (<italic>P<sub>L</sub></italic> and <italic>P<sub>A</sub></italic>) to quantify asymmetry in leaf area distributions of <italic>S</italic>. <italic>chinensis</italic>. By analyzing 480 shoots, we showed that 99.8% of RRLCs were left-skewed (<italic>S</italic> &lt; 1 and <italic>P<sub>L</sub></italic> or <italic>P<sub>A</sub></italic> &gt; 0.5), indicating a dominant role of larger leaves in driving inequality. These findings not only validate the utility of the performance equation in modeling RRLCs but also highlight the limitations of the Gini coefficient as a summary statistic of the Lorenz curve. The explicit relationship between <italic>S</italic> and <italic>P<sub>L</sub></italic> (<italic>S</italic> = 2 − 2<italic>P<sub>L</sub></italic>), alongside the empirical link between <italic>P<sub>L</sub></italic> and <italic>P<sub>A</sub></italic>, provides a robust toolkit for dissecting asymmetric patterns in biological size distributions. Below, we contextualize these results within three key themes: ecological implications of asymmetric resource allocation, methodological advancements in inequality metrics, and practical applications for plant ecology and management.</p><sec id="sec4dot1-plants-14-01345" disp-level="2"><title>4.1. Ecological Implications of Asymmetric Leaf Area Distributions and Resource Allocation Strategies</title><p>The finding that most RRLCs were left-skewed (<italic>S</italic> &lt; 1 and <italic>P<sub>L</sub></italic> or <italic>P<sub>A</sub></italic> &gt; 0.5) highlights the predominant contribution of larger leaves to the inequality of leaf area distributions of <italic>S</italic>. <italic>chinensis</italic> shoots. This asymmetry is consistent with ecological strategies for optimizing light capture in heterogeneous environments. The Lorenz asymmetry coefficient (<italic>S</italic>), originally proposed by Damgaard and Weiner [<xref rid="B19-plants-14-01345" ref-type="bibr">19</xref>], quantifies the contribution of large-size individuals to the inequality of size distributions, a metric now complemented by two novel measures, <italic>P<sub>L</sub></italic> and <italic>P<sub>A</sub></italic>, for the RRLC. In shaded understories or lower canopy layers, plants often develop larger, thinner leaves to maximize light interception [<xref rid="B4-plants-14-01345" ref-type="bibr">4</xref>,<xref rid="B5-plants-14-01345" ref-type="bibr">5</xref>,<xref rid="B6-plants-14-01345" ref-type="bibr">6</xref>]. The observed left-skewed RRLCs may reflect adaptive basipetal gradients in leaf area, where older basal leaves expand to prolong photosynthetic activity under diminishing light availability, while younger apical leaves prioritize structural efficiency [<xref rid="B10-plants-14-01345" ref-type="bibr">10</xref>]. Such patterns suggest that bamboo shoots balance carbon investment across leaf ages to mitigate light limitation, a strategy critical for understory survival. Future studies could integrate light microclimate data (e.g., canopy openness) with leaf traits (e.g., specific leaf area, chlorophyll content) to test whether left-skewed distributions correlate with shade adaptation or nutrient reallocation dynamics.</p></sec><sec id="sec4dot2-plants-14-01345" disp-level="2"><title>4.2. Methodological Advancements: From the Gini Coefficient to Multidimensional Asymmetry Metrics</title><p>While the Gini coefficient provides a good overall measure of inequality, it lacks sensitivity to the asymmetry of Lorenz curves [<xref rid="B19-plants-14-01345" ref-type="bibr">19</xref>]. The Lorenz asymmetry coefficient <italic>S</italic> addressed this limitation by incorporating the contribution of large-size individuals to the Gini coefficient [<xref rid="B19-plants-14-01345" ref-type="bibr">19</xref>]. Building on this framework, our study introduces <italic>P<sub>L</sub></italic> and <italic>P<sub>A</sub></italic>, which leverage geometric properties of the RRLC to quantify its asymmetry through distinct approaches: <italic>P<sub>L</sub></italic> reflects the positional shift of the RRLC’s maximum value point, while <italic>P<sub>A</sub></italic> integrates the area ratio between the left and right parts of the performance curve intersecting with the <italic>x</italic>-axis. These metrics enhance the resolution of the analysis of inequality by disentangling the roles of outlier leaves (e.g., dominant apical leaves) versus cumulative small-leaf effects. The performance equation (Equation (2)), with parameters <italic>K</italic><sub>1</sub> and <italic>K</italic><sub>2</sub> governing curvature asymmetry, offers a flexible tool for modeling both discrete and continuous distributions. Notably, the strong relationship between <italic>P<sub>A</sub></italic> and <italic>P<sub>L</sub></italic> (<italic>r</italic><sup>2</sup> = 0.982) suggests redundancy in some applications but underscores their complementary utility in capturing different facets of asymmetry. Future work could extend this framework to other plant traits (e.g., seed mass and root biomass) and explore linkages to functional trade-offs, such as growth-defense balances [<xref rid="B12-plants-14-01345" ref-type="bibr">12</xref>].</p></sec><sec id="sec4dot3-plants-14-01345" disp-level="2"><title>4.3. Practical Applications and Future Directions: Bridging Theory and Management</title><p>The three asymmetry measures (<italic>S</italic>, <italic>P<sub>L</sub></italic>, and <italic>P<sub>A</sub></italic>) hold promise for ecological monitoring and management. For instance, in bamboo cultivation, shifts in <italic>P<sub>L</sub></italic> values could indicate stress responses, e.g., nutrient limitation might amplify left-skewed distributions as plants prioritize fewer large leaves for light foraging. Conversely, right-skewed patterns (<italic>S</italic> &gt; 1 or <italic>P<sub>L</sub></italic> and <italic>P<sub>A</sub></italic> &lt; 0.5) might signal intense intraspecific competition, favoring smaller leaves to reduce self-shading. While the performance equation exhibited robust fits (RMSE<sub>adj</sub> &lt; 0.05 for 98.1% of the 480 shoots), its primary value lies in enabling precise parameterization of RRLCs rather than directly diagnosing anomalies. Integrating these metrics with remote sensing (e.g., UAV-based multispectral imaging) could scale analyses to canopy levels, facilitating real-time assessments of leaf distribution health. However, the current study’s focus on a single species in a uniform habitat limits our ability to generalize. Future research should validate these methods across diverse taxa (e.g., broadleaf trees and grasses) and environments (e.g., tropical vs. temperate ecosystems). Additionally, linking asymmetry metrics to ecosystem functions, such as whether left-skewed distributions enhance carbon sequestration via dominant large leaves, could deepen our understanding of plant adaptation strategies under global change.</p></sec></sec><sec id="sec5-plants-14-01345" disp-level="1"><title>5. Conclusions</title><p>The Lorenz curve was originally developed to plot the cumulative percentage of household income (<italic>y</italic>′) against the cumulative percentage of number of households (<italic>x</italic>′) to reflect the inequality of income distributions. It has also been used to describe the inequality of biological size distributions. When the Lorenz curve is rotated counterclockwise by 135° and then shifted to the right by <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm34" overflow="scroll"><mml:mrow><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mrow></mml:math></inline-formula> (denoted as the rotated and right-shifted Lorenz curve, RRLC), it is a skewed or symmetrical bell-shaped curve that can be well described by a nonlinear equation (referred to as the performance equation), which has two intersections, (0, 0) and (<inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm35" overflow="scroll"><mml:mrow><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mrow></mml:math></inline-formula>, 0), with the <italic>x</italic>-axis. Double the area of the region formed by the performance curve and the <italic>x</italic>-axis equals the Gini coefficient, quantifying the overall inequality. Because the performance curve might be left-skewed, right-skewed, or symmetrical, which correspond to three size distribution patterns: (i) abundant large individuals contribute most to the inequality of size distributions, (ii) a few large individuals contribute most, and (iii) small-size and large-size individuals contribute equally. However, the Gini coefficient itself cannot reflect these three patterns exhibited by the Lorenz curve. Damgaard and Weiner [<xref rid="B19-plants-14-01345" ref-type="bibr">19</xref>] proposed an indicator for measuring the asymmetry of the Lorenz curve named the Lorenz asymmetry coefficient (<italic>S</italic>), which was defined as <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm36" overflow="scroll"><mml:mrow><mml:mrow><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm37" overflow="scroll"><mml:mrow><mml:mrow><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm38" overflow="scroll"><mml:mrow><mml:mrow><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mrow></mml:math></inline-formula> are the horizontal and vertical coordinates of the point at which the tangent of the Lorenz curve is a 45° straight line. The cases of <italic>S</italic> &lt; 1, <italic>S</italic> &gt; 1, and <italic>S</italic> = 1 exactly correspond to the above three size distribution patterns. In the present study, we provided another expression of the Lorenz asymmetry coefficient based on the RRLC, which is defined as the proportion of the line segment from (0, 0) to the point on the <italic>x</italic>-axis associated with the maximum value on the RRLC to <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm39" overflow="scroll"><mml:mrow><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mrow></mml:math></inline-formula>, denoted as <italic>P<sub>L</sub></italic>. It provides a more intuitive measure that has an explicit mathematical relationship with <italic>S</italic>, that is, <italic>S</italic> = 2 − 2<italic>P<sub>L</sub></italic>. In addition, a third asymmetry measure for the RRLC was proposed, which is defined as the area of the region formed by the left part of the RRLC and the <italic>x</italic>-axis to the area of the region formed by the whole RRLC and the <italic>x</italic>-axis, denoted as <italic>P<sub>A</sub></italic>. These three measures can reflect the contribution of the largest individuals to the overall inequality. Future studies should validate the prevalence of left-skewed leaf area distributions across plant species with contrasting ecological strategies (e.g., shade-tolerant vs. pioneer species), particularly under varying light and nutrient regimes. Additionally, investigating linkages between whole-plant morphological traits (e.g., aboveground biomass, height, and crown architecture) and the proposed asymmetry metrics (<italic>P<sub>L</sub></italic> and <italic>P<sub>A</sub></italic>) could elucidate how interspecific and intraspecific competition shapes leaf functional trait allocation, potentially through alterations in branching patterns, vertical growth, and canopy expansion, to optimize resource acquisition in heterogeneous environments.</p></sec><sec id="ack1" sec-type="ack" disp-level="1"><title>Acknowledgments</title><p>We thank Qiying Li, Meng Lian, Weihao Yao, and Liuyue Zhang for their work in leaf sampling and data acquisition. We also thank the three expert reviewers for their invaluable comments.</p></sec><sec id="app1-plants-14-01345" sec-type="app" disp-level="1"><title>Supplementary Materials</title><p>The following supporting information can be downloaded at <ext-link xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="https://www.mdpi.com/article/10.3390/plants14091345/s1" ext-link-type="uri">https://www.mdpi.com/article/10.3390/plants14091345/s1</ext-link>: Table S1: Estimated parameters, goodness of fit, and measures for the Lorenz curve’s asymmetry.</p><supplementary-material id="plants-14-01345-s001" position="float"><media xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="plants-14-01345-s001.zip" mimetype="application" mime-subtype="zip"><?cloudpmc-path 0d8d/12073621/36cb66d43f6b/plants-14-01345-s001.zip?><?cloudpmc-bucket app?><?size 129230?></media></supplementary-material></sec><sec id="app2-plants-14-01345" sec-type="app" disp-level="1"><title>Appendix A. Relationship Between Two Asymmetry Measures</title><p>It is apparent that the maximum value point <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm40" overflow="scroll"><mml:mrow><mml:mrow><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mo> </mml:mo><mml:msub><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mrow></mml:math></inline-formula> in the <italic>x–y</italic> plane is obtained by rotating <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm41" overflow="scroll"><mml:mrow><mml:mrow><mml:mfenced separators="|"><mml:mrow><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>,</mml:mo><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced></mml:mrow></mml:mrow></mml:math></inline-formula> counterclockwise by 3/4π and shifting it to the right by <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm42" overflow="scroll"><mml:mrow><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mrow></mml:math></inline-formula>. Thus, the following is obtained:</p><disp-formula id="FD10-plants-14-01345"><label>(A1)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm43" display="block" overflow="scroll"><mml:mrow><mml:mrow><mml:mfenced open="{" close="" separators="|"><mml:mrow><mml:mtable><mml:mtr><mml:mtd><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>−</mml:mo><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mfenced><mml:mrow><mml:mrow><mml:mi mathvariant="normal">cos</mml:mi></mml:mrow><mml:mo>⁡</mml:mo><mml:mrow><mml:mstyle scriptlevel="0" displaystyle="true"><mml:mfrac><mml:mrow><mml:mn>3</mml:mn></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>π</mml:mi></mml:mrow></mml:mrow><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mrow><mml:mi mathvariant="normal">sin</mml:mi></mml:mrow><mml:mo>⁡</mml:mo><mml:mrow><mml:mstyle scriptlevel="0" displaystyle="true"><mml:mfrac><mml:mrow><mml:mn>3</mml:mn></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>π</mml:mi></mml:mrow></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:mo>−</mml:mo><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>−</mml:mo><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow></mml:mfenced><mml:mrow><mml:mrow><mml:mi mathvariant="normal">sin</mml:mi></mml:mrow><mml:mo>⁡</mml:mo><mml:mrow><mml:mstyle scriptlevel="0" displaystyle="true"><mml:mfrac><mml:mrow><mml:mn>3</mml:mn></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>π</mml:mi></mml:mrow></mml:mrow><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mrow><mml:mi mathvariant="normal">cos</mml:mi></mml:mrow><mml:mo>⁡</mml:mo><mml:mrow><mml:mstyle scriptlevel="0" displaystyle="true"><mml:mfrac><mml:mrow><mml:mn>3</mml:mn></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>π</mml:mi></mml:mrow></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mfenced><mml:mo>.</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula><p>
Because <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm44" overflow="scroll"><mml:mrow><mml:mrow><mml:mrow><mml:mrow><mml:mi mathvariant="normal">sin</mml:mi></mml:mrow><mml:mo>⁡</mml:mo><mml:mrow><mml:mstyle scriptlevel="0" displaystyle="true"><mml:mfrac><mml:mrow><mml:mn>3</mml:mn></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>π</mml:mi></mml:mrow></mml:mrow><mml:mo>=</mml:mo><mml:mstyle scriptlevel="0" displaystyle="true"><mml:mfrac><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm45" overflow="scroll"><mml:mrow><mml:mrow><mml:mrow><mml:mrow><mml:mi mathvariant="normal">cos</mml:mi></mml:mrow><mml:mo>⁡</mml:mo><mml:mrow><mml:mstyle scriptlevel="0" displaystyle="true"><mml:mfrac><mml:mrow><mml:mn>3</mml:mn></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:mfrac></mml:mstyle><mml:mi>π</mml:mi></mml:mrow></mml:mrow><mml:mo>=</mml:mo><mml:mo>−</mml:mo><mml:mstyle scriptlevel="0" displaystyle="true"><mml:mfrac><mml:mrow><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mrow></mml:math></inline-formula> we obtain the following:</p><disp-formula id="FD11-plants-14-01345"><label>(A2)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm46" display="block" overflow="scroll"><mml:mrow><mml:mrow><mml:mi>S</mml:mi><mml:mo>=</mml:mo><mml:msubsup><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:mn>2</mml:mn><mml:mo>−</mml:mo><mml:msqrt><mml:mn>2</mml:mn></mml:msqrt><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo>.</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula><p> According to the definition of <italic>P<sub>L</sub></italic> (Equation (6)), we obtain the following:</p><disp-formula id="FD12-plants-14-01345"><label>(A3)</label><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="mm47" display="block" overflow="scroll"><mml:mrow><mml:mrow><mml:mi>S</mml:mi><mml:mo>=</mml:mo><mml:mn>2</mml:mn><mml:mo>−</mml:mo><mml:mn>2</mml:mn><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>L</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:math></disp-formula></sec><sec id="notes1" disp-level="1"><title>Author Contributions</title><p>Methodology, C.F.D., P.S. and J.W.; formal analysis, Y.C. and P.S.; investigation, F.J.; supervision, P.S. and J.W.; writing—original draft preparation, Y.C. and P.S.; writing—review and editing, C.F.D. and J.W. All authors have read and agreed to the published version of the manuscript.</p></sec><sec id="notes2" disp-level="1"><title>Institutional Review Board Statement</title><p>Not applicable.</p></sec><sec id="notes3" disp-level="1"><title>Informed Consent Statement</title><p>Not applicable.</p></sec><sec id="notes4" disp-level="1"><title>Data Availability Statement</title><p>The raw data of leaf size measures are available in the online Supplementary Tables S1 and S3 in ref. [<xref rid="B31-plants-14-01345" ref-type="bibr">31</xref>].</p></sec><sec id="notes5" disp-level="1"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest.</p></sec><sec id="funding-statement1" xml:lang="en" disp-level="1"><title>Funding Statement</title><p>This research itself received no external funding.</p></sec><sec id="fn-group1" sec-type="fn-group" disp-level="1"><title>Footnotes</title><fn-group><fn id="fn1"><p><bold>Disclaimer/Publisher’s Note:</bold> The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). 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