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  <front>
    <journal-meta>
      <journal-id journal-id-type="nlm-ta">Iontronics</journal-id>
      <journal-id journal-id-type="publisher-id">ions</journal-id>
      <journal-title-group>
        <journal-title>Iontronics</journal-title>
      </journal-title-group>
      <issn pub-type="epub">3070-6483</issn>
      <publisher>
        <publisher-name>OAE Publishing Inc.</publisher-name>
      </publisher>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.20517/iontronics.2026.22</article-id>
      <article-id pub-id-type="publisher-id">IONS-2026-22</article-id>
      <article-categories>
        <subj-group>
          <subject>Perspective</subject>
        </subj-group>
      </article-categories>
      <title-group>
        <article-title>Breaking ionic-strength barriers in contact-electro-catalysis</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes">
          <name>
            <surname>Wang</surname>
            <given-names>Ziming</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
          <xref ref-type="aff" rid="I2">
            <sup>2</sup>
          </xref>
          <xref ref-type="aff" rid="I3">
            <sup>3</sup>
          </xref>
          <xref ref-type="aff" rid="I1035">
            <sup>#</sup>
          </xref>
          <xref ref-type="aff" rid="I1042">
            <sup>*</sup>
          </xref>
          <xref ref-type="corresp" rid="cor1">*</xref>
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>Dai</surname>
            <given-names>Quanbin</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
          <xref ref-type="aff" rid="I2">
            <sup>2</sup>
          </xref>
          <xref ref-type="aff" rid="I1035">
            <sup>#</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>Jiang</surname>
            <given-names>Dongjian</given-names>
          </name>
          <xref ref-type="aff" rid="I3">
            <sup>3</sup>
          </xref>
          <xref ref-type="aff" rid="I4">
            <sup>4</sup>
          </xref>
          <xref ref-type="aff" rid="I1035">
            <sup>#</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author" corresp="yes">
          <name>
            <surname>Xia</surname>
            <given-names>Zhenhai</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
          <xref ref-type="aff" rid="I2">
            <sup>2</sup>
          </xref>
          <xref ref-type="aff" rid="I1042">
            <sup>*</sup>
          </xref>
          <xref ref-type="corresp" rid="cor1">*</xref>
        </contrib>
      </contrib-group>
      <aff id="I1"><sup>1</sup>ARC Centre of Excellence for Carbon Science and Innovation, University of New South Wales, Sydney 2052, Australia.</aff>
      <aff id="I2"><sup>2</sup>School of Chemical Engineering, University of New South Wales, Sydney 2052 Australia.</aff>
      <aff id="I3"><sup>3</sup>Center for High-Entropy Energy and Systems, Beijing Institute of Nanoenergy and Nanosystems, Chinese Academy of Sciences, Beijing 101400, China.</aff>
      <aff id="I4"><sup>4</sup>School of Nanoscience and Engineering, University of Chinese Academy of Sciences; Beijing 100049, China.</aff>
      <aff id="I1035"><sup>#</sup>These authors contributed equally to this work.</aff>
      <author-notes>
        <corresp id="cor1"><sup id="I1042">*</sup>Correspondence to: Prof. Zhenhai Xia ARC Centre of Excellence for Carbon Science and Innovation, University of New South Wales, Sydney 2052, Australia; School of Chemical Engineering, University of New South Wales, Sydney 2052 Australia. E-mail: <email>zhenhai.xia@unsw.edu.au</email>; Dr. Ziming Wang, ARC Centre of Excellence for Carbon Science and Innovation, University of New South Wales, Sydney 2052, Australia; School of Chemical Engineering, University of New South Wales, Sydney 2052 Australia; Center for High-Entropy Energy and Systems, Beijing Institute of Nanoenergy and Nanosystems, Chinese Academy of Sciences, Beijing 101400, China. E-mail: <email>ziming.wang14@unsw.edu.au</email></corresp>
        <fn fn-type="other">
          <p><bold>Received:</bold> 2 Jun 2026 | <bold>First Decision:</bold> 25 Jun 2026 | <bold>Revised:</bold> 21 Jul 2026 | <bold>Accepted:</bold> 22 Jul 2026 | <bold>Published:</bold> 13 Aug 2026</p>
        </fn>
      </author-notes>
      <pub-date pub-type="ppub">
        <year>2026</year>
      </pub-date>
      <pub-date pub-type="epub">
        <day>13</day>
        <month>8</month>
        <year>2026</year>
      </pub-date>
      <volume>2</volume>
	  <issue>3</issue>
      <elocation-id>27</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>
    </article-meta>
  </front>
  <body>
      <p>Contact-electrification (CE) is a ubiquitous surface phenomenon in which two surfaces become oppositely charged after repeated contact and separation<sup>[<xref ref-type="bibr" rid="B1">1</xref>,<xref ref-type="bibr" rid="B2">2</xref>]</sup>. Electrons have often been identified as the dominant charge carrier in the CE process<sup>[<xref ref-type="bibr" rid="B3">3</xref>-<xref ref-type="bibr" rid="B5">5</xref>]</sup>, and an electron-cloud-potential-well model has been proposed for the CE-driven electron transfer<sup>[<xref ref-type="bibr" rid="B2">2</xref>,<xref ref-type="bibr" rid="B6">6</xref>]</sup>. Based on the CE effect under mechanical stimuli, contact-electro-catalysis (CEC) has emerged as a novel catalytic strategy to promote chemical reactions<sup>[<xref ref-type="bibr" rid="B7">7</xref>-<xref ref-type="bibr" rid="B9">9</xref>]</sup>. CEC has provided sustainable and effective means for environmental remediation<sup>[<xref ref-type="bibr" rid="B10">10</xref>,<xref ref-type="bibr" rid="B11">11</xref>]</sup>, vital chemical synthesis<sup>[<xref ref-type="bibr" rid="B12">12</xref>,<xref ref-type="bibr" rid="B13">13</xref>]</sup>, and resource recovery<sup>[<xref ref-type="bibr" rid="B14">14</xref>,<xref ref-type="bibr" rid="B15">15</xref>]</sup>. However, most reported CEC processes have been limited to low-ionic-strength media, largely because ion transfer competes with electron transfer during CE<sup>[<xref ref-type="bibr" rid="B16">16</xref>-<xref ref-type="bibr" rid="B18">18</xref>]</sup>. As a result, the electron transfer process can be significantly suppressed at high ion concentrations<sup>[<xref ref-type="bibr" rid="B19">19</xref>,<xref ref-type="bibr" rid="B20">20</xref>]</sup>, leading to substantially reduced CEC efficiency. Given the abundance of mobile ions in realistic aqueous environments, it is highly desirable to develop efficient CEC platforms that can efficiently operate under high-ionic-strength conditions.</p>
      <p>In this Perspective, we first analyze the competition between electron transfer and ion transfer during liquid-solid CE and discuss how this competition limits CEC under high-ionic-strength conditions. We then highlight microenvironment engineering as a promising strategy for regulating ion distributions at the contact interfaces to mitigate their adverse effects on CE and subsequent catalytic processes. Finally, we envision the opportunities enabled by CEC across a broader ionic-strength window. Specifically, integrating CEC with electrocatalysis in an electrolyte could generate synergistic effects to greatly enhance overall performance for many promising applications in realistic aqueous environments, including hydrogen production from seawater, and beyond. Besides, we expect that a deeper understanding of the roles of surface-bound ions and adsorbates may inspire future CEC systems in which ions become active participants in catalytic reactions. The overall framework is illustrated in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p>
      <fig id="fig1" position="float">
        <label>Figure 1</label>
        <caption>
          <p>Contact-electro-catalysis across a broad ionic-strength window: challenges, solutions, and opportunities. CEC: Contact-electro-catalysis; DFT: density functional theory; EC: contact-electrification.</p>
        </caption>
        <graphic xlink:href="iontronics2022.fig.1.jpg"/>
      </fig>
    <sec id="sec1">
      <title>CHALLENGES IN HIGH IONIC STRENGTH CONDITIONS</title>
      <p>Liquid-solid contact-electrification (L-S CE) occurs spontaneously when a solid contacts a liquid. Recent studies suggest that both electrons and ions participate in interfacial charge transfer during L-S CE<sup>[<xref ref-type="bibr" rid="B21">21</xref>-<xref ref-type="bibr" rid="B23">23</xref>]</sup>, with electrons dominating in many cases, particularly at hydrophobic surfaces and under low-ionic-strength conditions<sup>[<xref ref-type="bibr" rid="B3">3</xref>,<xref ref-type="bibr" rid="B24">24</xref>]</sup>. An electron-cloud-potential-well model has been established to describe the CE-driven electron transfer process for redox reactions via CEC<sup>[<xref ref-type="bibr" rid="B2">2</xref>,<xref ref-type="bibr" rid="B7">7</xref>]</sup>. However, ion transfer arising from ion adsorption or ionization reactions could compete with electron transfer during L-S CE, thereby reducing the efficiency of CEC, especially in high-ionic-strength media. </p>
      <p>In addition, CE-induced surface charging may also modify wetting behavior and other interfacial interactions, which could further influence subsequent CEC efficiencies<sup>[<xref ref-type="bibr" rid="B25">25</xref>,<xref ref-type="bibr" rid="B26">26</xref>]</sup>. For example, a charged solid surface formed after CE tends to attract oppositely charged species from the surrounding solutions. Such electrostatic adsorption has been visualized in previous CEC studies<sup>[<xref ref-type="bibr" rid="B7">7</xref>,<xref ref-type="bibr" rid="B27">27</xref>]</sup>. For example, positively charged powders (e.g., Nylon-66) would become yellowish after ultrasonicating in a methyl orange (MO) aqueous solution due to electrostatic adsorption of anionic methyl orange<sup>[<xref ref-type="bibr" rid="B9">9</xref>]</sup>. Such ion accumulation can negatively affect CEC in at least two ways: (1) it hinders further electron transfer during subsequent CE events, thereby reducing the number of electrons for catalytic reactions; and (2) its formation of an electrical double layer (EDL) would shield the charged surface, weakening the CE-derived electric field that facilitates substrate activation. Consequently, the overall CEC efficiency is substantially limited under high-ionic-strength conditions.</p>
    </sec>
    <sec id="sec2">
      <title>SOLUTIONS FOR ENHANCING CEC IN HIGH-IONIC-STRENGTH LIQUIDS</title>
      <p>Given the decisive role of ion adsorption in limiting CEC performance, microenvironment engineering at the contact interface offers a promising route for enhancing CEC in high-ionic-strength liquids. The primary objective is to regulate the spatial distribution of ions and prevent their excessive accumulation in regions where CEC occurs. A representative example is the construction of hydrogen bond networks (HBNs) at the contact surface.  Recent studies have suggested that HBN could limit the negative impact of ion accumulation on the CEC efficiency by regulating the ion spatial distribution near the contact region<sup>[<xref ref-type="bibr" rid="B14">14</xref>]</sup>. Specifically, hydrophobic fluorinated functional groups were first introduced on the hydrophilic surface of SiO<sub>2</sub> via a self-assembly strategy<sup>[<xref ref-type="bibr" rid="B28">28</xref>]</sup>. The synergetic interaction between the grafted fluorinated groups and surface hydroxyl groups then generated an HBN. This HBN remained stable under high-ionic-strength conditions (e.g., 0.5 M NaCl aqueous solution) and could prevent excessive accumulation of Na<sup>+</sup> and Cl<sup>-</sup> ions near contact surfaces<sup>[<xref ref-type="bibr" rid="B16">16</xref>]</sup>. As a result, ion-induced interference with CE-driven interfacial electron transfer was alleviated, while the shield effect of the CE-derived electric field was reduced, significantly improving the CEC efficiency even in ion-rich media. </p>
      <p>Surface modulation may also provide a feasible approach to regulate interfacial ion distribution, as certain ion species could be selectively repelled by tailored functional groups. Similarly, confinement using nanopores, nanochannels, or specific surface morphologies may reshape local ion distribution by creating low-ion buffering regions. Consequently, CE-driven electron transfer near the contact interface may be maintained even when the bulk solution is highly concentrated with ions.</p>
      <p>At a more fundamental level, it is essential to gain a deeper mechanistic understanding of how the nature of ions, ion concentration, and surface chemistry regulate CE at contact interfaces. In particular, ion adsorption is a dynamic and time-dependent process, and kinetic studies may inspire the development of ultrafast CEC strategies that minimize ion access to CE-active regions, thereby eliminating ion accumulation and the associated performance degradation. We expect in-situ characterization and density functional theory (DFT) calculations will facilitate such kinetic studies and help establish general design rules for CEC in high-ionic-strength environments.</p>
    </sec>
    <sec id="sec3">
      <title>OPPORTUNITIES IN REALISTIC AQUEOUS ENVIRONMENTS</title>
      <p>The development of CEC systems that maintain high efficiencies across a wide range of ionic strength could substantially broaden the practical applicability of CEC. In particular, industrial wastewater, environmental sewage, and municipal water streams often contain high concentrations of dissolved salts and charged pollutants. A CEC platform that remains effective under such conditions could therefore open new possibilities for direct industrial wastewater remediation, environmental water purification, tap water treatment, and many more.</p>
      <p>Covering more than 70% of the Earth’s surface, seawater represents another abundant and inherently ion-rich medium<sup>[<xref ref-type="bibr" rid="B29">29</xref>,<xref ref-type="bibr" rid="B30">30</xref>]</sup>. One particularly attractive application is its use as a feedstock for hydrogen production<sup>[<xref ref-type="bibr" rid="B31">31</xref>,<xref ref-type="bibr" rid="B32">32</xref>]</sup>. Compared with the increasing shortage of freshwater resources<sup>[<xref ref-type="bibr" rid="B33">33</xref>]</sup>, seawater is far more abundant and readily accessible, making it an appealing alternative for sustainable hydrogen generation. However, conventional polymer-based CEC catalysts often suffer an apparent decline in CE performance in saline solutions rich in Na<sup>+</sup> and Cl<sup>-</sup> due to the shielding effect of ions<sup>[<xref ref-type="bibr" rid="B33">33</xref>]</sup>. We anticipate that advanced CEC-based seawater hydrogen evolution platforms could not only reduce the reliance on scarce freshwater but also offer a sustainable route for <italic>in situ</italic> hydrogen production by converting unlimited mechanical energy from marine environments into electron transfer to drive the CEC process.</p>
      <p>The development of highly efficient CEC systems for high-salinity conditions could also enable their integration with electrocatalysis. More importantly, previous studies have demonstrated that the CE-derived high-intensity electric field on dielectric surfaces can polarize adjacent metallic catalysts, and thereby selectively promote their redox reactivities for certain reactions<sup>[<xref ref-type="bibr" rid="B34">34</xref>-<xref ref-type="bibr" rid="B35">35</xref>]</sup>. However, this CE-derived electric field would be significantly shielded by ions, especially in electrolytes with high ion concentrations essential for electrocatalysis. Consequently, the effective coupling of CEC and electrocatalysis remains challenging unless strategies are developed to suppress ion adsorption and interfacial screening. Once these challenges are addressed, this combination should render a significant improvement in both catalytic efficiency and selectivity, breaking the scaling rule in catalysis.</p>
    </sec>
    <sec id="sec4">
      <title>OUTLOOK</title>
      <p>High-ionic-strength media represent both a major challenge and a new opportunity for CEC. The challenge arises mainly from the coexistence of competitive electron transfer and ion transfer during L-S CE. While CE-driven electron transfer can accelerate target reactions, ion transfer can inhibit electron transfer without contributing to catalysis. Therefore, a key requirement for enhancing CEC under high-ionic-strength conditions is restricting ion transfer and accumulation at adjacent contact surfaces. </p>
      <p>Microenvironment engineering offers a promising strategy for regulating ion distribution and preventing excessive ion accumulation in regions where CE occurs. Recent studies have suggested that hydrogen bond networks (HBNs) can minimize the negative impact of ions by confining them to regions away from the contact interface. As ion transport and accumulation are dynamic processes, advanced in-situ characterization and DFT calculations are expected to facilitate kinetic studies to gain in-depth mechanistic understanding for developing novel strategies and establishing general design rules to improve CEC performance in high-ionic-strength environments.</p>
      <p>We envision that, once these challenges are addressed, CEC can be extended to realistic aqueous systems that are inherently rich in ions. This advancement would not only broaden the application scope of CEC, but also enable its integration with electrocatalysis in high-ionic-strength media. Such integration could generate synergistic effects for CEC and electrocatalysis to cooperatively enhance both the selectivity and efficiency of important chemical reactions, potentially breaking the scaling rule in catalysis. </p>
    </sec>
  </body>
  <back>
    <sec>
      <title>DECLARATIONS</title>
      <sec>
        <title>Authors’ contributions</title>
        <p>Conceptualization and writing: Wang, Z.; Jiang, D.; Dai, Q.</p>
        <p>Supervision: Xia, Z.; Wang, Z.</p>
        <p>Critical revision of the manuscript: Xia, Z.; Wang, Z.</p>
      </sec>
      <sec>
        <title>Availability of data and materials </title>
        <p>Not applicable.</p>
      </sec>
      <sec>
        <title>AI and AI-assisted tools statement</title>
        <p>Not applicable.</p>
      </sec>
      <sec>
        <title>Financial support and sponsorship</title>
        <p>Not applicable.</p>
      </sec>
      <sec>
        <title>Conflicts of interest</title>
        <p>The authors declared that there are no conflicts of interest.</p>
      </sec>
      <sec>
        <title>Ethical approval and consent to participate</title>
        <p>Not applicable.</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>
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