﻿<article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta>
      <journal-id journal-id-type="nlm-ta">Energy Mater.</journal-id>
      <journal-id journal-id-type="publisher-id">ENERGYMATER</journal-id>
      <journal-title-group>
        <journal-title>Energy Materials</journal-title>
      </journal-title-group>
      <issn pub-type="epub">2770-5900</issn>
      <publisher>
        <publisher-name>OAE Publishing Inc.</publisher-name>
      </publisher>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.20517/energymater.2026.182</article-id>
      <article-categories>
        <subj-group>
          <subject>Article</subject>
        </subj-group>
      </article-categories>
      <title-group>
        <article-title>Multifunctional organic molecules as electron-buffering layers for stabilizing Zn anodes</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <name>
            <surname>Yue</surname>
            <given-names>Qu</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
          <xref ref-type="aff" rid="I2">
            <sup>2</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>He</surname>
            <given-names>Junhui</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>Chen</surname>
            <given-names>Yuhang</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>Zhu</surname>
            <given-names>Huaipu</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>Gao</surname>
            <given-names>Taotao</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
          <xref ref-type="aff" rid="I3">
            <sup>3</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>Xiao</surname>
            <given-names>Dan</given-names>
          </name>
          <xref ref-type="aff" rid="I4">
            <sup>4</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author" corresp="yes">
          <name>
            <surname>Qiu</surname>
            <given-names>Lu</given-names>
          </name>
          <xref ref-type="aff" rid="I5">
            <sup>5</sup>
          </xref>
          <xref ref-type="aff" rid="I*">
            <sup>*</sup>
          </xref>
          <xref ref-type="corresp" rid="cor1" />
        </contrib>
        <contrib contrib-type="author" corresp="yes">
          <name>
            <surname>Li</surname>
            <given-names>Xiaoqin</given-names>
          </name>
          <xref ref-type="aff" rid="I5">
            <sup>5</sup>
          </xref>
          <xref ref-type="aff" rid="I*">
            <sup>*</sup>
          </xref>
          <xref ref-type="corresp" rid="cor1" />
        </contrib>
      </contrib-group>
      <aff id="I1">
        <sup>1</sup>School of Mechanical Engineering, Chengdu University, Chengdu 610106, Sichuan, China.</aff>
      <aff id="I2">
        <sup>2</sup>Institute for Advanced Study, Chengdu University, Chengdu 610106, Sichuan, China.</aff>
      <aff id="I3">
        <sup>3</sup>Key Laboratory of Fruit Waste Treatment and Resource Recycling of the Sichuan Provincial College, Neijiang Normal University, Neijiang 641100, Sichuan, China.</aff>
      <aff id="I4">
        <sup>4</sup>College of Chemical Engineering, Sichuan University, Chengdu 610064, Sichuan, China.</aff>
      <aff id="I5">
        <sup>5</sup>College of Food and Biological Engineering, Chengdu University, Chengdu 610106, Sichuan, China.</aff>
      <author-notes>
        <corresp id="cor1"><sup>*</sup>Correspondence to: Prof. Lu Qiu, Xiaoqin Li, College of Food and Biological Engineering, Chengdu University, Chengdu 610106, Sichuan, China. E-mail: <email>qiulu@cdu.edu.cn</email>; <email>lixiaoqin@cdu.edu.cn</email></corresp>
        <fn fn-type="other">
          <p>
            <bold>Received:</bold> 21 Jun 2026 |  <bold>First Decision:</bold> 7 Jul 2026 |  <bold>Revised:</bold> 26 Jul 2026 | <bold>Accepted:</bold> 21 Aug 2026 |  <bold>Published:</bold> 13 Oct 2026</p>
        </fn>
        <fn fn-type="other">
          <p>
            <bold>Academic Editor:</bold> Bin Wang | <bold>Copy Editor:</bold> Ping Zhang | <bold>Production Editor:</bold> Ping Zhang</p>
        </fn>
      </author-notes>
	  <pub-date pub-type="ppub">
        <year>2026</year>
      </pub-date>
      <pub-date pub-type="epub">
        <day>13</day>
        <month>10</month>
        <year>2026</year>
      </pub-date>
      <volume>6</volume>
	  <issue>10</issue>
      <elocation-id>600132</elocation-id>
      <permissions>
        <copyright-statement>© The Author(s) 2026.</copyright-statement>
        <license xlink:href="https://creativecommons.org/licenses/by/4.0/">
          <license-p>© The Author(s) 2026. <bold>Open Access</bold> This article is licensed under a Creative Commons Attribution 4.0 International License (<uri xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</uri>), which permits unrestricted use, sharing, adaptation, distribution and reproduction in any medium or format, for any purpose, even commercially, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.</license-p>
        </license>
      </permissions>
      <abstract>
        <p>Interfacial instability at the Zn anode represents a major obstacle to the advancement <InlineParagraph>of aqueous zinc-ion</InlineParagraph> batteries (AZIBs), as it triggers nonuniform Zn deposition and <InlineParagraph>various parasitic reactions.</InlineParagraph> This study investigates the influence of alizarin red S (ARS), an organic molecule featuring an extended π-conjugated framework and multiple functional groups <InlineParagraph>(-SO<sub>3</sub><sup>-</sup>,</InlineParagraph> -OH, and -C=O), on the Zn anode/electrolyte interface. For comparison, sodium p-hydroxybenzenesulfonate (PHS) and sodium benzenesulfonate (SBS) were also investigated. Owing to the synergistic effect of the π-conjugated framework and functional groups, ARS preferentially adsorbs onto the Zn surface and acts as an electron-buffering layer, thereby homogenizing the local interfacial electron distribution and promoting uniform Zn deposition. Meanwhile, the electrochemical reduction of ARS generates a dense inorganic-rich solid electrolyte interphase, effectively suppressing nonuniform Zn growth and undesirable interfacial reactions. Spectroscopic analyses indicate that ARS primarily disrupts the hydrogen-bonding network of the electrolyte rather than altering the Zn<sup>2+</sup> solvation structure. At different current densities and capacities, Zn//Zn cells using the ZnSO<sub>4</sub> + ARS electrolyte exhibit longer cycle stability than those using ZnSO<sub>4</sub>, ZnSO<sub>4</sub> + PHS, and ZnSO<sub>4</sub> + SBS electrolytes. This study provides a rational design strategy for multifunctional electrolyte additives in high-performance AZIBs.</p>
      </abstract>
      <kwd-group>
        <kwd>Aqueous zinc ion batteries</kwd>
        <kwd>organic molecules</kwd>
        <kwd>interfacial adsorption</kwd>
        <kwd>electron-buffering layers</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec1">
      <title>INTRODUCTION</title>
      <p>Owing to their favorable safety profile, economic viability, and reduced environmental impact, aqueous zinc-ion batteries (AZIBs) are suited for large-scale energy storage and could complement existing lithium-ion battery technologies<sup>[<xref ref-type="bibr" rid="B1">1</xref>,<xref ref-type="bibr" rid="B2">2</xref>]</sup>. Studies have demonstrated that interfacial engineering plays a crucial role in enhancing the performance of Zn-based energy storage systems, including alkaline Zn-air batteries<sup>[<xref ref-type="bibr" rid="B3">3</xref>-<xref ref-type="bibr" rid="B5">5</xref>]</sup>. Nevertheless, the interfacial challenges in AZIBs differ substantially because they involve Zn deposition/stripping in ZnSO<sub>4</sub>-based electrolytes, which are accompanied by dendrite growth and parasitic side reactions<sup>[<xref ref-type="bibr" rid="B6">6</xref>,<xref ref-type="bibr" rid="B7">7</xref>]</sup>. To address interfacial issues, researchers have recently proposed various strategies to regulate metal-ion deposition behavior and interfacial reaction kinetics, including catalytic interfacial engineering<sup>[<xref ref-type="bibr" rid="B8">8</xref>-<xref ref-type="bibr" rid="B11">11</xref>]</sup>, electrolyte optimization<sup>[<xref ref-type="bibr" rid="B12">12</xref>,<xref ref-type="bibr" rid="B13">13</xref>]</sup>, interface engineering and electrode structure design<sup>[<xref ref-type="bibr" rid="B14">14</xref>-<xref ref-type="bibr" rid="B17">17</xref>]</sup>. Recent studies have demonstrated that catalytic interfacial engineering can accelerate Zn<sup>2+</sup> desolvation, lower the nucleation barrier, and regulate Zn deposition kinetics<sup>[<xref ref-type="bibr" rid="B10">10</xref>,<xref ref-type="bibr" rid="B18">18</xref>]</sup>. Alongside catalytic interface design, electrolyte engineering has also emerged as an effective approach for tailoring the Zn anode/electrolyte interface and suppressing parasitic side reactions. For example, Na<sup>+</sup><sup>[<xref ref-type="bibr" rid="B19">19</xref>]</sup>, Mg<sup>2+</sup><sup>[<xref ref-type="bibr" rid="B20">20</xref>]</sup>, and Y<sup>3+</sup><sup>[<xref ref-type="bibr" rid="B21">21</xref>]</sup> ions were introduced into the electrolytes. Due to their adsorption on the Zn anode surface, the craze growth of Zn dendrites was inhibited by the formation of shielding layers. However, owing to the irreversible depletion of the inorganic salt additive, the prolonged cycling performance of AZIBs needs to be further demonstrated.</p>
      <p>Organic molecule additives, encompassing both small molecules and polymers (e.g., esters, nitriles, amines), have received considerable research attention<sup>[<xref ref-type="bibr" rid="B22">22</xref>-<xref ref-type="bibr" rid="B24">24</xref>]</sup>. This is primarily attributed to the ability of heteroatom-based functional groups (e.g., -S-, -N-, C=O, and C=N) to coordinate with Zn<sup>2+</sup> ions via their lone electron pairs, thereby modulating the solvation of the Zn<sup>2+</sup> ions<sup>[<xref ref-type="bibr" rid="B25">25</xref>]</sup>. Besides, introducing organic additives into the electrolyte can lower the activity of H<sub>2</sub>O molecules and hinder their redox reactions due to the strong binding to H<sub>2</sub>O molecules<sup>[<xref ref-type="bibr" rid="B26">26</xref>]</sup>. It has been reported that short-chain alcohols, such as ethanol and erythritol, can penetrate the Zn<sup>2+</sup> solvation sheath via interactions with coordinated H<sub>2</sub>O, altering the primary solvation structure of Zn<sup>2+</sup><sup>[<xref ref-type="bibr" rid="B27">27</xref>]</sup>. Ether additives have been shown to form a shielding layer at the Zn protrusion tip, thereby directing Zn<sup>2+</sup> deposition into adjacent depressions and yielding a smoother zinc deposit morphology<sup>[<xref ref-type="bibr" rid="B28">28</xref>]</sup>. Moreover, extending the carbon chain length and increasing the number of functional groups within the additive molecules reinforce the hydrogen-bonding network with H<sub>2</sub>O, thereby suppressing undesirable side reactions. However, the incorporation of organic additives is not without drawbacks, as it may compromise the electrolyte’s ionic conductivity and potentially impair battery safety. Therefore, a judicious balance between the type and concentration of additives is essential to achieve optimal electrochemical performance.</p>
      <p>As a result, trace-based organic molecular additives have received attention<sup>[<xref ref-type="bibr" rid="B29">29</xref>-<xref ref-type="bibr" rid="B32">32</xref>]</sup>. For instance, Yu <italic>et al.</italic> introduced trace amounts of hexamethylenetetramine (HMTA) as additives into the electrolyte of AZIBs. The HMTA additives can preferentially adsorb onto the Zn anode surface, creating a unique anode-molecule interface<sup>[<xref ref-type="bibr" rid="B29">29</xref>]</sup>. On the other hand, organic molecular additives based on bifunctional groups have been investigated<sup>[<xref ref-type="bibr" rid="B6">6</xref>,<xref ref-type="bibr" rid="B33">33</xref>]</sup>. For example, Li <italic>et al.</italic> reported the use of 4-amino-benzene-sulfonic acid (ABSA) additives in the ZnSO<sub>4</sub> electrolyte to improve the performance of AZIBs<sup>[<xref ref-type="bibr" rid="B6">6</xref>]</sup>. They observed that ABSA forms an adsorption layer on the Zn anode surface, thereby facilitating the formation of a stable, sulfur-rich solid electrolyte interphase (SEI). In addition, organic molecules containing both sulfonic acid groups and hydroxyl or carbonyl groups have attracted considerable attention owing to their bifunctional characteristics<sup>[<xref ref-type="bibr" rid="B26">26</xref>,<xref ref-type="bibr" rid="B34">34</xref>]</sup>. Sun <italic>et al.</italic> proposed a chemical self-deoxygenation strategy involving the addition of sodium anthraquinone-2-sulfonate into the electrolyte, which effectively mitigates the performance degradation of AZIBs induced by dissolved oxygen<sup>[<xref ref-type="bibr" rid="B35">35</xref>]</sup>. However, the underlying mechanism by which the functional groups of organic additives regulate Zn deposition and stripping remains to be fully elucidated.</p>
      <p>On this basis, alizarin red S (ARS) organic molecules bearing sulfonic acid, hydroxyl, and carbonyl groups were selected as electrolyte additives in this work. Their interactions with both the Zn anode interface and the electrolyte bulk were investigated. Comparative investigations were carried out on sodium p-hydroxybenzenesulfonate (PHS), which contains both hydroxyl and sulfonic groups, and sodium benzenesulfonate (SBS), which contains only a sulfonic group. Although similar multifunctional organic additives have been studied for Zn anode stabilization through Zn<sup>2+</sup> coordination<sup>[<xref ref-type="bibr" rid="B36">36</xref>]</sup>, preferential adsorption<sup>[<xref ref-type="bibr" rid="B6">6</xref>]</sup>, and solvation regulation<sup>[<xref ref-type="bibr" rid="B34">34</xref>]</sup>, relatively little attention has been paid to exploiting organic molecules with extended π-conjugated frameworks to regulate the interfacial electron distribution. Results show that, with the synergistic effect of the extended π-conjugated framework and multiple functional groups, ARS molecules can adsorb onto the Zn anode surface, homogenizing the local interfacial electron density and achieving uniform Zn deposition. Meanwhile, the C=O groups in ARS can accept protons, mitigating local pH fluctuations and effectively suppressing the accumulation of parasitic products. In addition, the electrochemical reduction of ARS generates a dense inorganic-rich SEI <italic>in situ</italic> at the Zn/electrolyte interface. Such an interfacial layer homogenizes Zn<sup>2+</sup> flux and improves the reversibility of Zn deposition/dissolution. Benefiting from these effects, symmetric Zn//Zn cells containing ARS sustain prolonged operation beyond 2,700 h (1 mA cm<sup>-2</sup>, 0.5 mAh cm<sup>-2</sup>) and 2,000 h (2 mA cm<sup>-2</sup>, 1 mAh cm<sup>-2</sup>), exceeding those cells using ZnSO<sub>4</sub>, ZnSO<sub>4</sub> + PHS, and ZnSO<sub>4</sub> + SBS electrolytes. Zn//I<sub>2</sub> batteries using the ZnSO<sub>4</sub> + ARS electrolyte also deliver superior cycling stability and rate performance compared with those using the ZnSO<sub>4</sub> electrolyte. This work provides new insights into the design of high-performance AZIBs through the use of multifunctional additive molecules.</p>
    </sec>
    <sec id="sec2">
      <title>EXPERIMENTAL AND COMPUTATIONAL METHODS</title>
      <sec id="sec2-1">
        <title>Materials</title>
        <p>ARS (IND), PHS (98%), SBS (98%), and ZnSO<sub>4</sub>·7H<sub>2</sub>O (99%) were purchased from Shanghai Yuanye Bio-Technology Co., Ltd. Activated carbon (AC), I<sub>2</sub>, N-methyl-2-pyrrolidone (NMP, 99%), and polyvinylidene difluoride (PVDF) were provided by Shanghai Macklin Biochemical Co., Ltd. Zn foil (50 μm, 99.999%) and Ti foil (20 μm, 99.999%) were provided by Institute for High Purity Metallic Materials. The glass fiber separator (260 μm) was obtained from GE Whatman. Acetylene black was obtained from Shandong Xiya Chemical Co., Ltd.</p>
      </sec>
      <sec id="sec2-2">
        <title>Electrolytes and cells</title>
        <p>The electrolytes used in this work are pure ZnSO<sub>4</sub> (2 M) and ZnSO<sub>4</sub> (2 M) with 0.02 mM additives, including ARS, PHS, and SBS, respectively. The optimal concentration of 0.02 mM was chosen to avoid the severe corrosion caused by a more acidic electrolyte at higher additive loadings [<inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 1</inline-supplementary-material>]. Ti//Zn cells and Zn//Zn cells were fabricated using commercial Ti foil and Zn foil without treatment and Whatman glass microfiber. Before assembling the Zn//I<sub>2</sub> cells, the cathode material was prepared by diffusing iodine into the activated carbon and heating it at 90 °C for 4 h (I<sub>2</sub>:AC = 3:7). Then, a homogeneous cathode slurry was obtained by dispersing the cathode material, acetylene black, and PVDF (8:1:1 by weight) in NMP. Zn//I<sub>2</sub> batteries were assembled using the as-prepared cathode and Zn foil as the cathode and anode, respectively, separated by glass fiber. The mass of iodine was nearly 1.0 mg cm<sup>-2</sup>. All cells were assembled into CR2032 coin cells.</p>
      </sec>
      <sec id="sec2-3">
        <title>Characterizations</title>
        <p>A JEOL JEM-F200 (Japan) and a Hitachi SU8100 (Japan) were employed for Transmission Electron Microscopy (TEM) and Scanning Electron Microscopy (SEM) observations, respectively. X-ray Photoelectron Spectroscopy (XPS) measurements were obtained with a Thermo Scientific K-Alpha (USA). <sup>1</sup>H Nuclear Magnetic Resonance (NMR) spectra were acquired on a Bruker Avance NEO 600 MHz spectrometer (Germany). Infrared spectra were collected using a Thermo Scientific Nicolet iN10 Fourier Transform Infrared Spectrometer (FTIR, USA). Raman spectroscopy tests were conducted using WITec alpha300 R (Germany). The crystalline structures were examined using Cu-Kα radiation on a Bruker D8 ADVANCE diffractometer (Bruker AXS GmbH, Germany), with an operating voltage of 40 kV and a scanning 2θ window of 5-80°. Ultravilet-visible (UV-Vis) Spectroscopy tests were analyzed using a Shimadzu UV1900i plus (Japan). <italic>In situ</italic> optical measurements were performed using Motic BA310Met microscopy (China).</p>
        <p>The electrochemical cycling performance was tested on an Autolab M204 workstation (Metrohm, Switzerland). The cells and batteries’ charge/discharge and rate performance were tested on a Neware BTS-51 battery testing system (Neware, Shenzhen, China). A conventional three-electrode setup was employed for Tafel and cyclic voltammetry (CV) measurements, with Zn foil serving as the working electrode, Ti foil as the counter electrode, and Ag/AgCl as the reference electrode. The additive-induced variation in the electric double-layer (EDL) capacitance was investigated separately by CV in Zn//Zn symmetric cells. Hydrogen evolution behavior in the presence of the additive was examined through the linear scan voltammetry (LSV) measurements of symmetric Zn//Zn cells. For impedance analysis, electrochemical impedance spectroscopy (EIS) spectra were acquired under open-circuit potential (OCP) conditions by applying a 5 mV AC perturbation across the frequency range of 0.01 Hz ~100 kHz.</p>
      </sec>
      <sec id="sec2-4">
        <title>Theoretical calculation</title>
        <p>Density functional theory (DFT) calculations were conducted with the DMol3 program package available in Materials Studio to quantify the intermolecular binding and adsorption energetics. The molecular structures were fully optimized using the generalized gradient approximation and Perdew-Burke-Ernzerhof exchange-correlation functional, followed by the corresponding energy calculations. The total orbital truncation parameter was set to 5.2 Å. The convergence criteria for orbital occupancy and energy were defined as 5 × 10<sup>-3</sup> and 1 × 10<sup>-5</sup> Ha, respectively, while the maximum force and atomic displacement were limited to 0.002 Ha Å<sup>-1</sup> and 0.005 Å, respectively. The binding energy (E<sub>bind</sub>) between the ARS, PHS, SBS, H<sub>2</sub>O, and Zn<sup>2+</sup> was calculated according to<sup>[<xref ref-type="bibr" rid="B37">37</xref>]</sup>:</p>
        <p><disp-formula> <label>(1)</label> <tex-math id="E1"> $$ \mathrm{ E_{bind}} = \mathrm{E_{Total}} – (\mathrm{E_{A}} + \mathrm{E_{B}}) $$ </tex-math></disp-formula></p>
        <p>Where E<sub>Total</sub> is the whole system’s energy. E<sub>A</sub> is the energy of ARS, PHS, and SBS, respectively. E<sub>B</sub> is the energy of the Zn<sup>2+</sup> or H<sub>2</sub>O molecule.</p>
        <p>The Zn (002) slab with lattice constants of 13.3245 Å × 13.3245 Å × 24.9468 Å was constructed to calculate the adsorption energy. A vacuum spacing of 20 Å was introduced along the direction normal to the slab to minimize interactions between periodic images. Brillouin-zone sampling was performed using a 1 × 1 × 1 k-point mesh. During structural optimization, the bottom-layer atoms were constrained at their initial positions, whereas the remaining upper atoms were allowed to relax. The adsorption strength of each species on the Zn (002) surface was quantified by the adsorption energy (E<sub>ads</sub>), defined as:</p>
        <p><disp-formula> <label>(2)</label> <tex-math id="E2"> $$ \mathrm{ E_{ads}} = \mathrm{E_{{slab + s}}} – (\mathrm{E_{slab}} + \mathrm{E_{s}}) $$ </tex-math></disp-formula></p>
        <p>where E<sub>slab+s</sub> denotes the total energy of the optimized adsorption system, and E<sub>slab</sub> and E<sub>s</sub> represent the energies of the pristine Zn (002) slab and the isolated adsorbate, respectively.</p>
      </sec>
    </sec>
    <sec id="sec3">
      <title>RESULTS AND DISCUSSION</title>
      <p>The three organic molecules differ in their functional groups: ARS contains -SO<sub>3</sub><sup>-</sup>, -OH, and -C=O groups; PHS contains -SO<sub>3</sub><sup>-</sup> and -OH groups; and SBS contains only -SO<sub>3</sub><sup>-</sup> group [<xref ref-type="fig" rid="fig1">Figure 1A</xref>]. Among them, ARS possesses an extended π-conjugated framework, PHS features a combination of intra-ring π-conjugation and p-π conjugation, whereas SBS is limited to intra-ring π-conjugation. Therefore, the electron regulation capability of the three molecules follows the order: ARS &gt; PHS &gt; SBS, attributed to the dimensionality of their π-conjugation systems. As a result, these molecules exhibit distinct effects on the Zn<sup>2+</sup> solvation sheath, Zn<sup>2+</sup> coordination environment, and hydrogen-bonding network within the electrolyte. As shown in <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figures 2</inline-supplementary-material>-<inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">4</inline-supplementary-material>, UV-Vis spectra of ARS-, PHS-, and SBS-containing ZnSO<sub>4</sub> electrolytes exhibit progressively intensified absorption bands with increasing additive concentration, indicating the increasing population of electronically active species in the electrolyte. Notably, the absorption band centered at ~525 nm is significantly enhanced in the ZnSO<sub>4</sub> + ARS electrolyte [<xref ref-type="fig" rid="fig1">Figure 1B</xref> and <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 2</inline-supplementary-material>]. This band is associated with the intramolecular charge transfer (ICT) transition within the anthraquinone π-conjugated framework of ARS<sup>[<xref ref-type="bibr" rid="B38">38</xref>,<xref ref-type="bibr" rid="B39">39</xref>]</sup>. The enhanced visible-light absorption suggests strengthened π-electron delocalization and electronic redistribution of ARS molecules induced by Zn<sup>2+</sup> interaction. In <xref ref-type="fig" rid="fig1">Figure 1B</xref>, the absorption band at ~262 nm related to the π → π* transition of the anthraquinone conjugate exhibits an obvious red shift<sup>[<xref ref-type="bibr" rid="B40">40</xref>,<xref ref-type="bibr" rid="B41">41</xref>]</sup>, which further indicates that the electron transition energy within the ARS framework is reduced and the π-electron delocalization is enhanced. Such electronically reconstructed ARS species possess an enhanced electron redistribution capability, enabling a more homogeneous interfacial electron distribution on the Zn surface, and thereby promoting uniform Zn deposition<sup>[<xref ref-type="bibr" rid="B42">42</xref>]</sup>.</p>
      <fig id="fig1" position="float">
        <label>Figure 1</label>
        <caption>
          <p>(A) The molecular structure characteristics of ARS, PHS, and SBS; (B) UV-Vis spectra of ZnSO<sub>4</sub>, ZnSO<sub>4</sub> + ARS, and ARS, respectively; (C) NMR spectra, (D) Raman spectra, and (E) hydrogen-bonding ratio of ZnSO<sub>4</sub>, ZnSO<sub>4</sub> with ARS/PHS/SBS, and ARS <InlineParagraph>(0.02 mM</InlineParagraph> aqueous solution); The binding energy of (F) H<sub>2</sub>O and (G) Zn<sup>2+</sup> to H<sub>2</sub>O, ARS, PHS, and SBS, respectively. ARS: Alizarin red S; SBS: sodium benzenesulfonate; NMR: nuclear magnetic resonance; UV-Vis: ultraviolet-visible; PHS: sodium p-hydroxybenzenesulfonate.</p>
        </caption>
        <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="em60182.fig.1.jpg" />
      </fig>
      <p>NMR, FTIR, and Raman techniques were combined to investigate the Zn<sup>2+</sup> solvation structure and hydrogen-bonding network of electrolytes. As shown in <xref ref-type="fig" rid="fig1">Figure 1C</xref>, a significant chemical shift of <sup>1</sup>H appears after introducing ARS, PHS, and SBS into ZnSO<sub>4</sub> solutions, indicating the formation of a new hydrogen-bonding network. Compared with the ZnSO<sub>4</sub> solutions, the <sup>1</sup>H NMR signals of water molecules in ZnSO<sub>4</sub> + ARS and ARS solutions show a significant chemical shift toward a higher field, indicating an increased electron density around the proton nuclei and an enhanced shielding effect arising from the interaction between ARS molecules and H<sub>2</sub>O<sup>[<xref ref-type="bibr" rid="B43">43</xref>]</sup>. <xref ref-type="fig" rid="fig1">Figure 1D</xref> and <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 5</inline-supplementary-material> show Raman and FTIR spectra of ZnSO<sub>4</sub> with different additives. In comparison with the pure ZnSO<sub>4</sub> solution, the proportion of strong hydrogen bonding decreased, whereas that of the medium hydrogen bonding increased in the solution containing ARS, PHS, and SBS [<xref ref-type="fig" rid="fig1">Figure 1E</xref> and <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 6</inline-supplementary-material>]. In contrast, the proportion of weak hydrogen bonding remained nearly unchanged, with values of approximately 6%~7%. Among the tested solutions, the ARS solution exhibited the lowest proportion of strong hydrogen bonding (58.6%) and the highest proportion of medium hydrogen bonding (34.4%). These results indicate that ARS, PHS, and SBS additives perturb the original hydrogen-bonding network<sup>[<xref ref-type="bibr" rid="B44">44</xref>]</sup>. This modification of the deposition environment may suppress both the Zn dendritic growth and the hydrogen evolution reaction (HER).</p>
      <p>DFT calculations were performed to investigate the interactions of different molecules. The binding energies of ARS, PHS, SBS, and H<sub>2</sub>O molecules are all lower than the binding energy between H<sub>2</sub>O molecules [<xref ref-type="fig" rid="fig1">Figure 1F</xref>], suggesting that they can affect the hydrogen-bonding network and possibly also the solvation sheath. Moreover, the binding energies of ARS, PHS, and SBS with Zn<sup>2+</sup> are lower than those of H<sub>2</sub>O, indicating that these molecules can enter the solvation sheath and partially replace the coordinated water molecules [<xref ref-type="fig" rid="fig1">Figure 1G</xref>]. However, these additives are used at trace concentrations. Consequently, their impact on the solvation sheath is rather limited in this work<sup>[<xref ref-type="bibr" rid="B45">45</xref>]</sup>.</p>
      <p>A combination of theoretical simulations and experimental tests was jointly applied to elucidate how these molecules interact with and regulate the electrode interface. The charge densities calculated by DFT show that the O in H<sub>2</sub>O, ARS, PHS, and SBS molecules exhibit significant electronegativity [<inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 7</inline-supplementary-material>], indicating a strong tendency for their adsorption onto the Zn surface<sup>[<xref ref-type="bibr" rid="B6">6</xref>]</sup>. The electronegative groups in the electrostatic potential diagram confirm the adsorption sites of these molecules on the Zn electrode surface [<inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 8</inline-supplementary-material>]. <xref ref-type="fig" rid="fig2">Figure 2A</xref> and <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 9</inline-supplementary-material> demonstrate their adsorption energies on the Zn (002) surface in horizontal and vertical configurations. As can be seen, ARS, PHS, and SBS molecules show stronger adsorption than H<sub>2</sub>O molecules in both horizontal and vertical orientations on the Zn (002) surface, owing to the rich lone-pair electrons on their O atoms. When adsorbed horizontally on the Zn (002) surface, the adsorption strength follows the order of ARS (-4.38 eV) &gt; PHS (-3.46 eV) &gt; SBS (-3.02 eV). In contrast, the adsorption strength order is reversed for the vertically adsorbed configurations. This difference can be attributed to the extended planar π-conjugated framework of ARS, which provides a larger contact area with the Zn (002) surface in the horizontal adsorption configuration, thereby strengthening van der Waals interactions and π-Zn interactions and resulting in stronger adsorption. In addition, the multiple polar functional groups of ARS enhance its interfacial interactions with the Zn surface through electrostatic interactions and charge redistribution, while the horizontal adsorption configuration further reduces steric hindrance. Conversely, for vertical adsorption, the interaction is mainly governed by localized coordination between sulfonic acid groups and the Zn surface. Therefore, SBS molecules with smaller steric hindrance exhibit relatively stronger adsorption in this configuration. The charge density difference in <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figures 10</inline-supplementary-material> and <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">11</inline-supplementary-material> verify the strong interactions between these molecules and the Zn (002) surface, showing more pronounced interfacial charge redistribution than that induced by H<sub>2</sub>O adsorption<sup>[<xref ref-type="bibr" rid="B46">46</xref>]</sup>. Meanwhile, owing to its multiple polar groups, ARS induces stronger interfacial charge redistribution with the Zn (002) surface than PHS and SBS. These results confirm that ARS, PHS, and SBS additive molecules can construct molecular adsorption layers with different adsorption strengths on the anode surface. Among them, ARS exhibits the strongest adsorption capability in the horizontal adsorption configuration due to the synergistic effect of its extended π-conjugated framework and multiple functional groups, which enables effective regulation of Zn<sup>2+</sup> deposition behavior and HER kinetics at the Zn electrode interface.</p>
      <fig id="fig2" position="float">
        <label>Figure 2</label>
        <caption>
          <p>(A) The adsorption energies of horizontally oriented H<sub>2</sub>O, ARS, PHS, and SBS on Zn (002); (B) OCP curves and (C) EDL capacitance measured in pristine and additive-containing ZnSO<sub>4</sub> electrolytes; (D) LUMO - HOMO energy band gap and frontier molecular orbital distributions of H<sub>2</sub>O, ARS, PHS, and SBS molecules; (E) LSV and (F) Tafel polarization responses obtained under different electrolyte conditions; (G-K) HRTEM observations of cycled Zn from ARS-containing electrolyte and (L) corresponding EDX elemental maps. ARS: Alizarin red S; SBS: sodium benzenesulfonate; LUMO: lowest unoccupied molecular orbital; HOMO: highest occupied molecular orbital; OCP: open-circuit potential; EDL: electric double-layer; LSV: linear scan voltammetry; HRTEM: high-resolution transmission electron microscopy; EDX: energy-dispersive X-ray spectroscopy; HAADF: high-angle annular dark-field; PHS: sodium p-hydroxybenzenesulfonate.</p>
        </caption>
        <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="em60182.fig.2.jpg" />
      </fig>
      <p>In addition to the preliminary theoretical evaluation, the OCPs of Zn electrodes in different electrolytes were measured to provide experimental evidence for the adsorption of additive molecules on the Zn surface. As shown in <xref ref-type="fig" rid="fig2">Figure 2B</xref>, the OCP of the Zn electrode in the ZnSO<sub>4</sub> electrolyte initially decreases due to Zn dissolution and then gradually recovers as the Zn<sup>2+</sup> concentration at the Zn electrode interface reaches equilibrium<sup>[<xref ref-type="bibr" rid="B47">47</xref>]</sup>. However, the OCPs of the Zn electrodes in the ZnSO<sub>4</sub>-containing ARS, PHS, and SBS electrolytes show positive shifts, which are attributed to the special adsorption of these molecules on the Zn surface. The EDL capacitance of the Zn electrode in different electrolytes was measured to elucidate the effect of interfacial molecular adsorption on the EDL characteristics, as illustrated in <xref ref-type="fig" rid="fig2">Figure 2C</xref> and <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 12</inline-supplementary-material>. The EDL capacitance of the Zn electrode in ZnSO<sub>4</sub> solutions is about 245 μF cm<sup>-2</sup>. After introducing ARS, PHS, and SBS additives into the ZnSO<sub>4</sub> solutions, this value decreases to 23 μF cm<sup>-2</sup>, <InlineParagraph>74 μF cm<sup>-2</sup>,</InlineParagraph> and 87 μF cm<sup>-2</sup>, respectively. According to the capacitance equation, the capacitance is inversely proportional to the thickness of the EDL. The reduced differential capacitance observed in <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 13</inline-supplementary-material> is consistent with this conclusion<sup>[<xref ref-type="bibr" rid="B15">15</xref>]</sup>. These findings verify the adsorption of ARS, PHS, and SBS on the Zn anode, thereby modifying the EDL structure and regulating the interfacial properties of the Zn electrode.</p>
      <p>The lowest unoccupied molecular orbital (LUMO) and highest occupied molecular orbital (HOMO) characteristics were analyzed to gain insight into the electronic interactions between the molecules and the Zn surface. The tendency of a molecule to donate or accept electrons can be inferred from its HOMO and LUMO energy levels, respectively. The order of HOMO energy levels of ARS, PHS, SBS, and H<sub>2</sub>O molecules is H<sub>2</sub>O &lt; ARS &lt; SBS &lt; PHS [<xref ref-type="fig" rid="fig2">Figure 2D</xref>]. This indicates that these molecular additives preferentially donate electrons to the Zn surface compared with adsorbed H<sub>2</sub>O molecules<sup>[<xref ref-type="bibr" rid="B48">48</xref>]</sup>. The energy levels are consistent with the adsorption energy results mentioned above. The ARS molecules have the lowest LUMO energy level, meaning that the ARS molecules are very susceptible to accepting electrons from the Zn anode. This facilitates the preferential reduction of ARS, thereby suppressing the HER<sup>[<xref ref-type="bibr" rid="B49">49</xref>,<xref ref-type="bibr" rid="B50">50</xref>]</sup>. Moreover, results show that the orbital energy gap (ΔE = E<sub>LUMO</sub> - E<sub>HOMO</sub>) of these molecules in descending order is: H<sub>2</sub>O (6.99 eV) &gt; SBS (2.99 eV) &gt; PHS (2.90 eV) &gt; ARS (1.58 eV). The value of ΔE reflects the chemical reactivity of the molecule. ARS molecules exhibit the lowest ΔE, suggesting they are readily reduced on the Zn surface, thereby forming an SEI that regulates Zn<sup>2+</sup> deposition and protects the Zn anode from corrosion<sup>[<xref ref-type="bibr" rid="B49">49</xref>,<xref ref-type="bibr" rid="B51">51</xref>]</sup>. Compared with PHS and SBS molecules, the ARS molecule contains multiple electronegative O atoms, which withdraw electron density from the aromatic rings, thus decreasing their π-electron density and making them susceptible to electrochemical reduction. The carbonyl (C=O) groups of ARS are proposed to undergo electrochemical reduction, likely forming hydroxylated aromatic species through the consumption of surface-adsorbed hydrogen intermediates, thereby suppressing HER and promoting the formation of a dense and uniform SEI<sup>[<xref ref-type="bibr" rid="B52">52</xref>]</sup>. In addition, the minimal pH variation in <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 14</inline-supplementary-material> indicates that the ARS additive effectively mitigates local pH fluctuations at the Zn/electrolyte interface. <xref ref-type="fig" rid="fig2">Figure 2E</xref> shows that the resistance of HER increased after the addition of ARS, PHS, and SBS, indicating suppressed HER<sup>[<xref ref-type="bibr" rid="B53">53</xref>]</sup>. This conclusion is further supported by the corrosion curves in <xref ref-type="fig" rid="fig2">Figure 2F</xref>. To be specific, the Zn electrode in the ZnSO<sub>4</sub> electrolyte has a corrosion current of 1.78 mA cm<sup>-2</sup> and a negative corrosion potential of -0.952 V. After adding ARS, PHS, and SBS, the corrosion potential shows a positive shift and the corrosion current density shows a decrease, implying the positive effect of additives on anti-corrosion performance<sup>[<xref ref-type="bibr" rid="B15">15</xref>]</sup>. Notably, upon the addition of ARS to the electrolyte, the corrosion current decreases to 0.708 mA cm<sup>-2</sup>, while the corrosion potential shifts positively to -0.947 V. These changes may be attributed to the electrochemical reduction of ARS molecules. CV curves in <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 15</inline-supplementary-material> show that there is a reduction peak at -0.7 V in the ARS electrolytes. The reduction species on the electrode were investigated by TEM [<xref ref-type="fig" rid="fig2">Figure 2G</xref>-<xref ref-type="fig" rid="fig2">K</xref>]. Results show that the lattice fringes of ZnCO<sub>3</sub> (104), ZnS (111), ZnO (100), and ZnCO<sub>3</sub> (116) are present on the Zn electrode cycled in ZnSO<sub>4</sub> with ARS electrolytes<sup>[<xref ref-type="bibr" rid="B50">50</xref>,<xref ref-type="bibr" rid="B54">54</xref>]</sup>, indicating the formation of an inorganic-rich SEI layer, which is composed of ZnCO<sub>3</sub>, ZnS, and ZnO. Energy-dispersive X-ray spectroscopy (EDX) elemental maps in <xref ref-type="fig" rid="fig2">Figure 2L</xref> show that the elemental distributions of C, S, O, and Zn on the Zn electrode surface are uniform. Sparse crystalline domains are discernible on the Zn surface after cycling in the pristine ZnSO<sub>4</sub> electrolyte [<inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figures 16</inline-supplementary-material> and <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">17</inline-supplementary-material>], although its EDX elemental maps resemble those obtained in the presence of ARS. Upon introducing ARS, substantially more lattice fringes appear across the cycled Zn surface, indicative of enhanced interfacial product formation. These microscopic features support the formation of a compact and continuous inorganic-rich SEI induced by the ARS additive.</p>
      <p>To identify the chemical composition of the species on the Zn anode cycled in ZnSO<sub>4</sub> and ZnSO<sub>4</sub> + ARS electrolytes, XPS coupled with Ar<sup>+</sup> sputtering was applied. The variation of O, S, and C elements with sputtering time is depicted in <xref ref-type="fig" rid="fig3">Figure 3A</xref> and <xref ref-type="fig" rid="fig3">B</xref>. Deconvolution of the O 1s spectrum yields three components centered at 529.9, 531.6, and 533.6 eV, corresponding to Zn-O, C=O/S=O, and C-O/O-H species, respectively<sup>[<xref ref-type="bibr" rid="B16">16</xref>,<xref ref-type="bibr" rid="B55">55</xref>]</sup>. With increasing Ar<sup>+</sup> sputtering time, the peak at 529.9 eV gradually increases, whereas the peak at 533.6 eV gradually disappears. The enhanced Zn-O signal indicates the presence of ZnO on the Zn electrode, which is attributed to the decomposition of Zn<sub>4</sub>SO<sub>4</sub>(OH)<sub>6</sub>·5H<sub>2</sub>O generated during the parasitic corrosion reactions between dissolved oxygen/water and Zn<sup>[<xref ref-type="bibr" rid="B56">56</xref>]</sup>. In the S 2p spectra, the peak at 169.1 eV is assigned to SO<sub>4</sub><sup>2-</sup><sup>[<xref ref-type="bibr" rid="B57">57</xref>,<xref ref-type="bibr" rid="B58">58</xref>]</sup>. With increasing Ar<sup>+</sup> sputtering time, the characteristic ZnS peak at 162.0 eV gradually emerges for the Zn electrode cycled in the ZnSO<sub>4</sub> + ARS electrolyte, whereas no corresponding Zn-S signal is detected for the Zn electrode cycled in the ZnSO<sub>4</sub> electrolyte. The findings suggest that the adsorbed ARS additives undergo electrochemical reduction at the anode interface, leading to the formation of ZnS species within the SEI. The C 1s spectrum comprises contributions from C-H/C-C (284.8 eV), C-O (286.4 eV), and ZnCO<sub>3</sub> (288.9 eV), with the latter likely originating from reactions involving dissolved CO<sub>2</sub> and decomposition products of organic molecules<sup>[<xref ref-type="bibr" rid="B29">29</xref>,<xref ref-type="bibr" rid="B55">55</xref>]</sup>. For the Zn electrode cycled in ZnSO<sub>4</sub> electrolyte, prolonged Ar<sup>+</sup> sputtering eliminates the C-O-C signal and progressively weakens the ZnCO<sub>3</sub> component [<xref ref-type="fig" rid="fig3">Figure 3A</xref>]. In contrast, the signal intensity of ZnCO<sub>3</sub> increases obviously, indicating rich ZnCO<sub>3</sub> on the Zn electrode [<xref ref-type="fig" rid="fig3">Figure 3B</xref>]. The results show that the addition of ARS facilitates the formation of a uniform inorganic-rich SEI composed of ZnO, ZnS, ZnCO<sub>3</sub> on the zinc electrode surface, in good agreement with the TEM observations. This robust interphase effectively inhibits Zn corrosion while promoting homogeneous Zn deposition<sup>[<xref ref-type="bibr" rid="B50">50</xref>]</sup>.</p>
      <fig id="fig3" position="float" width="500">
        <label>Figure 3</label>
        <caption>
          <p>In-depth XPS analysis of O 1s, S 2p, and C 1s on the Zn anode after 20 cycles in (A) pristine and (B) ARS-containing ZnSO<sub>4</sub>; (C) The current-time curves of Zn//Zn cells and (D) the potential-time curves of Ti//Zn cells in pristine and additive-containing ZnSO<sub>4</sub> electrolytes; (E) The corresponding SEM results; The influences of (F) pristine and (G) ARS-containing ZnSO<sub>4</sub> electrolytes on the Zn electrode surface. XPS: X-ray photoelectron spectroscopy; ARS: alizarin red S; SBS: sodium benzenesulfonate; SEI: solid electrolyte interphase; SEM: scanning electron microscopy; PHS: sodium p-hydroxybenzenesulfonate.</p>
        </caption>
        <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="em60182.fig.3.jpg" />
      </fig>
      <p>The chronoamperometry (CA) method was further applied to investigate the Zn nucleation and growth behavior. A lower steady-state current density indicates a more uniform and compact Zn deposition process, thereby suppressing dendrite formation<sup>[<xref ref-type="bibr" rid="B59">59</xref>]</sup>. <xref ref-type="fig" rid="fig3">Figure 3C</xref> demonstrates that the current density in the ZnSO<sub>4</sub> electrolytes increases continuously for 200 s until 25 mA cm<sup>-2</sup>. The current density during Zn deposition in ZnSO<sub>4</sub> electrolytes containing ARS, PHS, or SBS increases rapidly to about 17 mA cm<sup>-2</sup> within 100 s and remains stable thereafter. The rapid increase in current means the 3D diffusion process, while the slow increase in current means the 2D diffusion process<sup>[<xref ref-type="bibr" rid="B46">46</xref>]</sup>. The former results in uniform and dense Zn deposition, while the latter results in irregular and sparse Zn deposition. <xref ref-type="fig" rid="fig3">Figure 3D</xref> shows an increased Zn nucleation overpotential after the introduction of ARS, PHS, and SBS additives, meaning that these additives promote the formation of smaller Zn nuclei and refined Zn deposition, which results in a more uniform Zn plating/stripping process and highly reversible Zn anodes<sup>[<xref ref-type="bibr" rid="B60">60</xref>]</sup>.</p>
      <p>
        <italic>In situ</italic> optical microscopy was used to track the dynamic Zn deposition process at the electrode interface. After 20 min of plating, pronounced uneven Zn accumulation can be observed on the electrode surface [<inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 18</inline-supplementary-material>], indicating highly nonuniform Zn growth. However, Zn electrodes cycled in ZnSO<sub>4</sub> electrolytes containing ARS, PHS, or SBS exhibited smooth surfaces without obvious surface protrusions. The SEM results are consistent with this [<xref ref-type="fig" rid="fig3">Figure 3E</xref>]. Haphazard accumulation of large-sized flake deposits can be observed on the surface of Zn cycled in ZnSO<sub>4</sub> electrolytes. Due to the presence of ARS additives, the deposits on the Zn electrode are dense and uniform. For the Zn electrode cycled in the PHS-containing electrolyte, relatively uniform deposits are observed, although their particle size is considerably larger. Cycling in the presence of SBS leads to the formation of a porous and noncompact deposit on the Zn surface. The X-ray diffraction (XRD) profile of Zn retrieved from the additive-free <InlineParagraph>ZnSO<sub>4</sub> electrolyte</InlineParagraph> contains distinct reflections at 15°, 16°, 24°, and 31.5°, which are characteristic of <InlineParagraph>Zn<sub>4</sub>SO<sub>4</sub>(OH)<sub>6</sub>·5H<sub>2</sub>O</InlineParagraph> (JCPDS No. 39-0688) and ZnSO<sub>3</sub>·2.5H<sub>2</sub>O (JCPDS No. 42-0097) [<inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 19</inline-supplementary-material>]. Comparable by-product-related peaks are likewise present in the PHS-containing system. However, after introducing ARS and SBS into the electrolyte, the characteristic diffraction peaks of the by-products at 15° and 31.5° are no longer observed, and the intensities of the remaining diffraction peaks are substantially reduced. Taken together, these observations reveal highly nonuniform Zn deposition in the pristine ZnSO<sub>4</sub> electrolyte, characterized by pronounced surface irregularities and a heterogeneous deposit layer. However, owing to the interfacial regulation induced by the ARS, PHS, and SBS additives, Zn electrodes cycled in the corresponding additive-containing electrolytes exhibit smoother and more uniform Zn deposits. Among them, the ARS-containing electrolyte enables the formation of the densest and most homogeneous Zn deposition layer with minimal by-product formation.</p>
      <p>Based on the above theoretical calculations and experimental results, the mechanism of ARS additives for Zn anodic protection is suggested. In the ZnSO<sub>4</sub> electrolyte [<xref ref-type="fig" rid="fig3">Figure 3F</xref>], the Zn anode suffers from severe parasitic corrosion and hydrogen evolution, together with uncontrolled Zn dendritic growth, resulting in rapid deterioration of cycling performance. Upon introducing ARS into the electrolyte [<xref ref-type="fig" rid="fig3">Figure 3G</xref>], the preferential adsorption of ARS on the Zn anode surface displaces interfacial H<sub>2</sub>O molecules, creating a water-deficient interfacial environment. The C=O groups on the aromatic backbone of ARS preferentially react with surface-adsorbed hydrogen intermediates, thereby suppressing local alkalization caused by the HER. Subsequently, the adsorbed ARS molecules undergo electrochemical reduction to form a robust protective SEI. More importantly, due to the extended π-conjugated framework with highly delocalized π electrons, ARS acts as an electron-buffering layer that homogenizes the interfacial electron distribution on the Zn surface, thereby promoting uniform Zn deposition. Collectively, the introduction of ARS additives changes the Zn electrode interface by suppressing HER and Zn corrosion, facilitating reversible Zn deposition/stripping, and ultimately enhancing the cycling stability of the Zn anode.</p>
      <p>To access the effect on the cycling performance of Zn anodes, Zn//Zn cells using ZnSO<sub>4</sub> electrolytes with and without ARS, PHS, and SBS additives were tested at different current densities. <xref ref-type="fig" rid="fig4">Figure 4A</xref> shows that the Zn//Zn cell using the ZnSO<sub>4</sub> electrolyte experiences a sudden short circuit after 260 h of cycling at 1 mA cm<sup>-2</sup> and 0.5 mAh cm<sup>-2</sup>. With the introduction of additives, these cells can operate for more than 1,800 h. In particular, the Zn//Zn cell using the ZnSO<sub>4</sub> + ARS electrolyte exhibits stable cycling for over 2,700 h. At <InlineParagraph>2 mA cm<sup>-2</sup></InlineParagraph> with the capacity of 1 mAh cm<sup>-2</sup>, the cell using ZnSO<sub>4</sub> electrolytes shorts after 400 h of cycling, while the cell using ZnSO<sub>4</sub> with ARS, PHS, and SBS electrolytes can run for 2,000 h, 1,250 h, and 1,000 h, respectively [<xref ref-type="fig" rid="fig4">Figure 4B</xref>]. At 4 mAcm<sup>-2</sup> with the capacity of 1 mAh cm<sup>-2</sup>, the cell using ZnSO<sub>4</sub> + ARS electrolytes can cycle 1,800 h [<xref ref-type="fig" rid="fig4">Figure 4C</xref>]. At a high current density of 10 mA cm<sup>-2</sup> with the capacity of <InlineParagraph>10 mAh cm<sup>-2</sup>,</InlineParagraph> the cell with additives can also operate 230 h, longer than the cell with ZnSO<sub>4</sub> electrolytes (60 h) [<inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 20</inline-supplementary-material>]. In <xref ref-type="fig" rid="fig4">Figure 4D</xref>, the rate performance of Zn//Zn cells with the ZnSO<sub>4</sub> + ARS electrolyte shows favorable cycling stability under various current densities. Taken together, the Zn//Zn symmetric cells employing the ARS-containing electrolyte exhibit stable cycling over a wide range of current densities, demonstrating the robustness of the interfacial regulation effect under different operating conditions.</p>
      <fig id="fig4" position="float">
        <label>Figure 4</label>
        <caption>
          <p>Cycling behavior of symmetric Zn//Zn cells in pristine and additive-containing ZnSO<sub>4</sub> electrolytes at (A) 1, (B) 2, and (C) <InlineParagraph>4 mA cm<sup>-2</sup>;</InlineParagraph> (D) The rate performance of the cells over 1-5 mA cm<sup>-2</sup>; (E) Coulombic efficiency and (F) the corresponding initial potential-capacity curves of Ti//Zn cells with and without ARS at 1.0 mA cm<sup>-2</sup>. ARS: Alizarin red S; SBS: sodium benzenesulfonate; PHS: sodium p-hydroxybenzenesulfonate.</p>
        </caption>
        <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="em60182.fig.4.jpg" />
      </fig>
      <p>Zn plating/stripping reversibility was examined using Ti//Zn cells. The incorporation of ARS leads to a pronounced enhancement in Coulombic efficiency (CE), with an average value of 99.5% retained over 500 cycles [<xref ref-type="fig" rid="fig4">Figure 4E</xref>]. Without ARS, however, the average CE decreases to approximately 95%, and the cell survives for only 70 cycles, highlighting the beneficial role of ARS in stabilizing reversible Zn deposition. The reproducibility of the CE measurements was verified using three independently assembled Ti//Zn cells. The corresponding CE profiles and statistical analysis (99.46 ± 0.08, <italic>n</italic> = 3) are presented in <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 21</inline-supplementary-material>, confirming the excellent reproducibility of the electrochemical performance. The initial CE of the Ti//Zn cell using ZnSO<sub>4</sub> + ARS electrolytes is 95.05%, higher than that of the cell using ZnSO<sub>4</sub> electrolytes (90.02%) [<xref ref-type="fig" rid="fig4">Figure 4F</xref>], indicating that the irreversible loss of the former cell is smaller than that of the latter cell<sup>[<xref ref-type="bibr" rid="B61">61</xref>]</sup>. Conclusively, the excellent cycling stability of cells using ZnSO<sub>4</sub> + ARS electrolytes is associated with the formation of a suitable adsorption layer in the EDL structure and the inorganic-rich SEI protective layer on the Zn anode surface, which can modify the operating environment of the Zn anode.</p>
      <p>The significantly prolonged cycling lifespan of symmetric cells demonstrates the effectiveness of the electrolyte additives in suppressing Zn dendrite growth and the HER. To further verify the beneficial effect of the ARS additive in practical devices, Zn//I<sub>2</sub> full batteries were assembled. As shown in <xref ref-type="fig" rid="fig5">Figure 5A</xref>, introducing ARS additives into the ZnSO<sub>4</sub> electrolyte decreases the redox potential difference and increases the redox peak currents, indicating reduced electrochemical polarization and improved electrochemical reversibility. The EIS spectra in <xref ref-type="fig" rid="fig5">Figure 5B</xref> show that both the charge transfer resistance and interfacial resistance decrease upon the addition of ARS to the ZnSO<sub>4</sub> electrolyte, indicating accelerated interfacial charge transfer kinetics due to interfacial regulation induced by ARS adsorption.</p>
      <fig id="fig5" position="float">
        <label>Figure 5</label>
        <caption>
          <p>(A) CV profiles and (B) EIS spectra of the Zn//I<sub>2</sub> batteries in pristine and ARS-containing ZnSO<sub>4</sub> electrolytes; (C) Galvanostatic charge/discharge profiles of the ZnSO<sub>4</sub> + ARS electrolyte and (D) rate performance of the ZnSO<sub>4</sub> and ZnSO<sub>4</sub> + ARS electrolyte over a current-density range of 0.1-4.0 A g<sup>-1</sup>. Extended cycling behavior of Zn//I<sub>2</sub> batteries with and without ARS at (E) 0.2 A g<sup>-1</sup> and (F) 1.0 A g<sup>-1</sup>. CV: Cyclic voltammetry; EIS: electrochemical impedance spectroscopy; ARS: alizarin red S.</p>
        </caption>
        <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="em60182.fig.5.jpg" />
      </fig>
      <p>The galvanostatic charge/discharge profiles of Zn//I<sub>2</sub> batteries containing the ZnSO<sub>4</sub> electrolyte [<inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Figure 22</inline-supplementary-material>] and the ZnSO<sub>4</sub> + ARS electrolyte [<xref ref-type="fig" rid="fig5">Figure 5C</xref>] were collected over a wide range of current densities from 0.1 to 4.0 A g<sup>-1</sup>.  Their corresponding rate performance are presented in <xref ref-type="fig" rid="fig5">Figure 5D</xref>. Distinct voltage plateaus centered at approximately 1.3 V during charging and <InlineParagraph>1.2 V</InlineParagraph> during discharging are retained across these profiles, in good agreement with the redox features identified by CV. Compared with the battery using the ZnSO<sub>4</sub> electrolyte, the battery using ZnSO<sub>4</sub> + ARS electrolyte presents higher specific capacity and better rate performance. At 0.2 A g<sup>-1</sup>, it shows a capacity of <InlineParagraph>192 mAh g<sup>-1</sup></InlineParagraph> over 1,200 cycles with CE and capacity retention of 99.8% and 93%, respectively [<xref ref-type="fig" rid="fig5">Figure 5E</xref>]. The battery without ARS provides 174 mAh g<sup>-1</sup> under the same conditions, with its CE and capacity retention reaching 99.5% and 87%, respectively. The beneficial effect of ARS becomes particularly evident during extended cycling at 1.0 A g<sup>-1</sup>. Even beyond 7,000 cycles, a capacity of 170 mAh g<sup>-1</sup> is still accessible for the ARS-containing battery, substantially exceeding the 110 mAh g<sup>-1</sup> obtained with the pristine ZnSO<sub>4</sub> electrolyte [<xref ref-type="fig" rid="fig5">Figure 5F</xref>]. These results indicate that the stability of the Zn//I<sub>2</sub> full battery is enhanced over a wide range of current densities due to the improved interfacial regulation of the Zn anode by the ARS additives, highlighting its potential for practical applications.</p>
    </sec>
    <sec id="sec4">
      <title>CONCLUSION</title>
      <p>In this work, ARS organic molecules, featuring an extended π-conjugated framework and multiple functional groups (sulfonic acid, hydroxyl, and carbonyl groups), were employed as an electrolyte additive to regulate the Zn anode/electrolyte interface in AZIBs. Comparative investigations using PHS and SBS as reference additives revealed that the synergistic effect of the extended π-conjugated framework and multiple functional groups is crucial for effective interfacial regulation and stable Zn deposition. Combined experimental and theoretical investigations demonstrate that ARS adsorption homogenizes the local interfacial electron distribution, regulates the Zn<sup>2+</sup> flux, suppresses parasitic side reactions, and promotes the <italic>in situ</italic> formation of dense inorganic-rich SEI, thereby enabling uniform Zn deposition and highly reversible Zn plating/stripping. Consequently, Zn//Zn cells with the ZnSO<sub>4</sub> + ARS electrolyte exhibit stable cycling for more than 2,700 h at <InlineParagraph>1 mA cm<sup>-2</sup></InlineParagraph> (0.5 mAh cm<sup>-2</sup>) and 2,000 h at 2 mA cm<sup>-2</sup> (1 mAh cm<sup>-2</sup>), exceeding the cells with ZnSO<sub>4</sub>, ZnSO<sub>4</sub> + PHS, and ZnSO<sub>4</sub> + SBS electrolytes. The incorporation of ARS enables the Zn//I<sub>2</sub> full battery to achieve robust long-term cycling and favorable rate performance. This work provides a rational molecular design strategy for electrolyte additives by integrating an extended π-conjugated framework with multiple functional groups, offering new insights into interfacial regulation of Zn anodes for high-performance AZIBs.</p>
    </sec>
  </body>
  <back>
    <sec>
      <title>DECLARATIONS</title>
      <sec>
        <title>Acknowledgments</title>
        <p>The authors extend their gratitude to Ms. Mulan Chang (from Scientific Compass <uri xlink:href="http://www.shiyanjia.com">www.shiyanjia.com</uri>) for providing invaluable assistance with the XPS and NMR tests.</p>
      </sec>
      <sec>
        <title>Authors’ contributions</title>
        <p>Conceptualization, methodology, writing-original draft, formal analysis: Yue, Q.; He, J.</p>
        <p>Investigation, data curation, DFT calculation: He, J.; Chen, Y.; Zhu, H.</p>
        <p>Resources and supervision: Xiao, D.</p>
        <p>Funding acquisition: Gao, T.; Li, X.</p>
        <p>Project administration, supervision, writing-review: Qiu, L.; Li, X.</p>
      </sec>
      <sec>
        <title>Availability of data and materials</title>
        <p>The data supporting the findings of this study are available within the article and its <inline-supplementary-material content-type="local-data" mimetype="application/pdf" xlink:href="em60182-SupplementaryMaterials.pdf">Supplementary Materials</inline-supplementary-material>. Additional data are available from the corresponding author upon reasonable request.</p>
      </sec>
      <sec>
        <title>AI and AI-assisted tools statement</title>
        <p>Not applicable<bold>.</bold></p>
      </sec>
      <sec>
        <title>Financial support and sponsorship</title>
        <p>This work was funded by the Natural Science Foundation of Sichuan Province (No. 2025ZNSFSC0355) and the Key Laboratory of Fruit Waste Treatment and Resource Recycling of the Sichuan Provincial College (GZKF2405).</p>
      </sec>
      <sec>
        <title>Conflicts of interest</title>
        <p>All authors declared that there are no conflicts of interest.</p>
      </sec>
      <sec>
        <title>Ethical approval and consent to participate</title>
        <p>Not applicable<bold>.</bold></p>
      </sec>
      <sec>
        <title>Consent for publication</title>
        <p>Not applicable.</p>
      </sec>
      <sec>
        <title>Copyright</title>
        <p>© The Author(s) 2026.</p>
      </sec>
      <sec sec-type="supplementary-material">
        <title>Supplementary Materials</title>
        <supplementary-material content-type="local-data">
          <media xlink:href="em60182-SupplementaryMaterials.pdf" mimetype="application/pdf">
            <caption>
              <p>Supplementary Materials</p>
            </caption>
          </media>
        </supplementary-material>
      </sec>
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