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  <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.2026.30</article-id>
      <article-categories>
        <subj-group>
          <subject>Review</subject>
        </subj-group>
      </article-categories>
      <title-group>
        <article-title>Ion-concentration gradient electrolyte engineering in aqueous Zn-based batteries</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes">
          <name>
            <surname>Cui</surname>
            <given-names>Yifan</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
          <xref ref-type="aff" rid="I*">
            <sup>*</sup>
          </xref>
          <xref ref-type="corresp" rid="cor1" />
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>Jin</surname>
            <given-names>Zhenlong</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>Yu</surname>
            <given-names>Xinling</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author" corresp="yes">
          <name>
            <surname>He</surname>
            <given-names>Yi</given-names>
          </name>
          <xref ref-type="aff" rid="I2">
            <sup>2</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>Yang</surname>
            <given-names>Xulai</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</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 Advanced Manufacturing Engineering, LIB Technology Center of Anhui Province, Hefei University, Hefei 230601, Anhui, China.</aff>
      <aff id="I2">
        <sup>2</sup>Department of Chemical Engineering, Waterloo Institute for Nanotechnology, University of Waterloo, Waterloo, ON N2L 3G1 Canada.</aff>
      <author-notes>
        <corresp id="cor1">*Correspondence to: Dr. Yi He, Department of Chemical Engineering, Waterloo Institute for Nanotechnology, University of Waterloo, 200 University Avenue West, Waterloo, ON N2L 3G1 Canada. E-mail: <email>yi.he@uwaterloo.ca</email>; Dr. Yifan Cui, Dr. Xulai Yang, School of Advanced Manufacturing Engineering, LIB Technology Center of Anhui Province, Hefei University, Hefei 230601, Anhui, China. E-mail: <email>cuiyf@hfuu.edu.cn</email>; <email>yangxl@hfuu.edu.cn</email></corresp>
     
	  <fn fn-type="other">
          <p>
            <bold>Received:</bold> 7 Mar 2026 | <bold>First Decision:</bold> 16 Apr 2026 | <bold>Revised:</bold> 3 May 2026 | <bold>Accepted:</bold> 4 Jun 2026 | <bold>Published:</bold> 17 Jun 2026</p>
        </fn>
        <fn fn-type="other">
          <p>
            <bold>Academic Editor:</bold> Bin Wang | <bold>Copy Editor:</bold> Fangling Lan | <bold>Production Editor:</bold> Fangling Lan</p>
        </fn>
      </author-notes>
      <pub-date pub-type="ppub">
        <year>2026</year>
      </pub-date>
      <pub-date pub-type="epub">
        <day>17</day>
        <month>6</month>
        <year>2026</year>
      </pub-date>
      <volume>6</volume>
	  <issue>6</issue>
       <elocation-id>600063</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>Aqueous Zn-based batteries (AZBs) have attracted considerable attention as promising energy storage systems because of their intrinsic safety, low cost, and environmental friendliness. However, their practical application is limited by the instability of the Zn electrode interface, including uneven Zn deposition, hydrogen evolution, and other parasitic side reactions. These issues are closely related to the heterogeneous distribution of Zn<sup>2+</sup> ions and the resulting imbalance of interfacial reactions during cycling. Ion concentration gradient engineering has therefore emerged as an effective strategy to regulate Zn<sup>2+</sup> transport behavior and stabilize the Zn electrode interface. This review systematically summarizes recent advances in the construction of Zn<sup>2+</sup> concentration gradients in AZBs, covering both liquid and hydrogel electrolyte systems. Representative strategies, including functional electrolyte additives, ion-selective separators, asymmetric electrolyte configurations, gradient hydrogel networks, and additive-assisted hydrogel electrolytes, are discussed. These approaches demonstrate that spatial regulation of Zn<sup>2+</sup> concentration fields can fundamentally influence ion transport pathways, solvation and desolvation processes, electric double layer structures, and interfacial reaction kinetics, thereby homogenizing Zn<sup>2+</sup> flux, suppressing hydrogen evolution and dendrite growth, and improving the reversibility of Zn plating and stripping. In addition, recent progress in advanced characterization techniques, including electrochemically parameterized ion transport modelling, <italic>in situ</italic> ion concentration mapping, and fluorescence-based operando visualization, is needed to elucidate the dynamic evolution of Zn<sup>2+</sup> concentration gradients and their correlation with interfacial stability. Finally, general design principles, key challenges, and future perspectives for ion concentration gradient engineering are discussed, guiding the rational development of high-performance and durable AZBs.</p>
      </abstract>
      <kwd-group>
        <kwd>Aqueous Zn-based batteries</kwd>
        <kwd>quasi/all solid-state batteries</kwd>
        <kwd>Zn electrode</kwd>
        <kwd>gradient electrolyte</kwd>
        <kwd>advanced characterization</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec1">
      <title>INTRODUCTION</title>
      <p>Aqueous Zn-based batteries (AZBs) have emerged as among the most promising next-generation electrochemical energy-storage technologies, driven by the increasing demand for devices that are not only highly energy dense but also intrinsically safe, cost effective, and environmentally sustainable<sup>[<xref ref-type="bibr" rid="B1">1</xref>-<xref ref-type="bibr" rid="B4">4</xref>]</sup> [<xref ref-type="fig" rid="fig1">Figure 1</xref>]. Compared with lithium-, sodium-, and other metal-ion-based batteries employing flammable organic electrolytes, AZBs capitalize on the intrinsic nonflammability and benign nature of water, offering a significantly enhanced safety profile suitable for large-scale grid energy storage and consumer electronics applications<sup>[<xref ref-type="bibr" rid="B5">5</xref>-<xref ref-type="bibr" rid="B10">10</xref>]</sup>. Zn metal further has this advantage: it is earth abundant, inexpensive, and environmentally compatible, and it has a high theoretical capacity (820 mAh g<sup>-1</sup>) and low redox potential (-0.76 V <italic>vs</italic>. SHE)<sup>[<xref ref-type="bibr" rid="B11">11</xref>-<xref ref-type="bibr" rid="B13">13</xref>]</sup>. In addition, AZBs benefit from several practical advantages that make them particularly attractive for large-scale energy storage applications. The use of water-based electrolytes provides intrinsic safety compared with flammable organic electrolytes used in conventional lithium-ion batteries, significantly reducing the risks of thermal runaway and combustion. Zn is widely available in the Earth’s crust and can be produced at low cost through mature metallurgical processes, supported by a well-established industrial infrastructure for Zn mining, refining, and recycling. These features collectively enable potentially low manufacturing costs and strong sustainability for grid-scale energy storage technologies.</p>
      <fig id="fig1" position="float">
        <label>Figure 1</label>
        <caption>
          <p>Advantages of aqueous Zn-based batteries.</p>
        </caption>
        <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="em6030.fig.1.jpg" />
      </fig>
      <p>Despite these compelling advantages, several intrinsic scientific challenges still hinder the practical deployment and commercial scalability of AZBs, including dendrite formation<sup>[<xref ref-type="bibr" rid="B14">14</xref>-<xref ref-type="bibr" rid="B21">21</xref>]</sup>, electrode passivation<sup>[<xref ref-type="bibr" rid="B22">22</xref>-<xref ref-type="bibr" rid="B26">26</xref>]</sup>, and the hydrogen evolution reaction (HER)<sup>[<xref ref-type="bibr" rid="B27">27</xref>-<xref ref-type="bibr" rid="B33">33</xref>]</sup>. Among them, uncontrolled Zn dendrite formation stands out as a key bottleneck, as it can cause internal short circuits, compromise cycling stability, and raise serious safety concerns. The main strategies for suppressing dendrite formation can be divided into five types: (i) the construction of artificial solid electrolyte interface<sup>[<xref ref-type="bibr" rid="B34">34</xref>-<xref ref-type="bibr" rid="B39">39</xref>]</sup>, (ii) the incorporation of electrolyte additives<sup>[<xref ref-type="bibr" rid="B40">40</xref>-<xref ref-type="bibr" rid="B44">44</xref>]</sup>, (iii) the structural design of Zn electrodes<sup>[<xref ref-type="bibr" rid="B45">45</xref>-<xref ref-type="bibr" rid="B49">49</xref>]</sup>, (iv) the optimization of charging-discharging protocols<sup>[<xref ref-type="bibr" rid="B50">50</xref>-<xref ref-type="bibr" rid="B54">54</xref>]</sup>, and (v) the use of solid or hydrogel electrolytes<sup>[<xref ref-type="bibr" rid="B55">55</xref>-<xref ref-type="bibr" rid="B59">59</xref>]</sup>. For example, a porous nano-CaCO<sub>3</sub> coating on a Zn electrode surface can guide Zn<sup>2+</sup> deposition to occur evenly in the crevices among particles, enabling a 42.7% higher discharge capacity after 1,000 cycles than that of the bare Zn electrode (177 <italic>vs</italic>. <InlineParagraph>124 mAh g<sup>-1</sup></InlineParagraph> at <InlineParagraph>1 A g<sup>-1</sup>)<sup>[<xref ref-type="bibr" rid="B60">60</xref>]</sup>.</InlineParagraph> Additionally, a water-immiscible ionic liquid diluent can form a “water pocket” to suppress water activity, thereby mitigating the tip effect and reducing parasitic reactions<sup>[<xref ref-type="bibr" rid="B61">61</xref>]</sup>. When this additive was added to the electrolyte of the Zn-Zn<sub>0.5</sub>V<sub>2</sub>O<sub>5</sub>·nH<sub>2</sub>O battery, the battery could operate stably for 400 cycles at 60 °C, with a capacity retention greater than 85%. From a structural perspective, semiliquid Zn powder anodes mitigate plating-induced stress and increase the availability of active sites, supporting more than 5,000 stable cycles<sup>[<xref ref-type="bibr" rid="B49">49</xref>]</sup>. In addition, surface-structured Zn anodes homogenize Zn<sup>2+</sup> flux by reducing the local current density and using the laminar flow of an etchant solution, which reflects the obvious synergistic effect between electrode surface structure design and electrolyte gradient engineering<sup>[<xref ref-type="bibr" rid="B62">62</xref>]</sup>. Furthermore, a current-controlled electrodeposition strategy has been shown to regulate the crystallographic orientation of Zn. Increasing the current density from 20 to 80 mA cm<sup>-2</sup> induces a transition in the preferred growth plane from (101) to (002), with the (002) texture favouring more homogeneous Zn deposition<sup>[<xref ref-type="bibr" rid="B50">50</xref>,<xref ref-type="bibr" rid="B63">63</xref>]</sup>. Accordingly, full cells employing (002)-textured Zn anodes paired with V/Mn-based oxide cathodes exhibit improved cycling stability (Zn(002)-MnO<sub>2</sub> full cells have a reversible capacity of 206.1 mAh g<sup>-1</sup> after 200 cycles with <InlineParagraph>0.2 A g<sup>-1</sup>).</InlineParagraph></p>
      <p>Beyond the aforementioned Zn deposition regulation strategies, hydrogel electrolytes have emerged as effective platforms for stabilizing Zn plating/stripping behavior. Owing to their three-dimensional polymer networks, hydrogel electrolytes can simultaneously provide mechanical constraints and continuous ionic pathways, thereby reshaping the interfacial environment of Zn electrodes. For instance, multicrosslinked alkaline gel electrolytes demonstrate superior mechanical robustness and ionic conductivity, enabling batteries to operate stably under extreme conditions with high energy efficiency<sup>[<xref ref-type="bibr" rid="B64">64</xref>]</sup>. Beyond structural integrity, the molecular engineering of polymer side chains offers a precise means to dictate interfacial reactions. A notable example is the integration of heterocyclic tetrazole groups to create polymeric single-ion conductors, which achieve an exceptional Zn<sup>2+</sup> transference number of 0.94 and significantly extend the shelf life of Zn batteries<sup>[<xref ref-type="bibr" rid="B65">65</xref>]</sup>. Furthermore, introducing high-valent cations such as Zr<sup>4+</sup> into silk fibroin-based hydrogels not only reinforces the matrix but also guides epitaxial growth along the (002) plane, effectively suppressing parasitic side reactions even at high depths of discharge<sup>[<xref ref-type="bibr" rid="B66">66</xref>]</sup>. Collectively, these advancements underscore that the efficacy of interfacial strategies fundamentally hinges on “ion modulation”. By sophisticatedly tailoring the local solvation structure and transport kinetics, these approaches converge on a central design principle: the construction and regulation of the ion concentration gradient.</p>
      <p>To provide mechanistic insights into the stabilization of Zn electrode interfaces, this review systematically reviews state-of-the-art strategies for constructing Zn<sup>2+</sup> concentration gradients in aqueous Zn-based batteries, covering both liquid electrolytes and solid-state hydrogel electrolytes. In liquid systems, Zn<sup>2+</sup> concentration gradients are regulated through electrolyte chemistry, such as functional additives, and interfacial engineering approaches, including ion-selective separators, enabling the suppression of interfacial side reactions and the homogenization of ion flux<sup>[<xref ref-type="bibr" rid="B67">67</xref>]</sup>. In hydrogel systems, intrinsic ionic confinement within polymer networks introduces additional design flexibility, allowing gradient construction through tailored network architectures and spatially differentiated ionic environments<sup>[<xref ref-type="bibr" rid="B68">68</xref>]</sup>. By integrating these strategies, this review highlights that controlled Zn<sup>2+</sup> concentration fields fundamentally govern ion transport pathways, solvation and desolvation behavior, electric field distribution, and interfacial reaction kinetics. In this context, ion-concentration gradient engineering is distinguished from related concepts such as solvation structure regulation and general interfacial modification by treating the spatial distribution of Zn<sup>2+</sup> as a primary and independent design parameter. While solvation regulation operates at the molecular scale and interfacial engineering focuses on surface stabilization, gradient engineering functions at the mesoscopic scale by deliberately constructing spatially nonuniform Zn<sup>2+</sup> distributions, thereby establishing chemical potential gradients that directly regulate ion flux and deposition behavior. Importantly, solvation modulation and interfacial control can act as enabling mechanisms for gradient formation but do not inherently generate spatial asymmetry unless specifically designed. Therefore, ion-concentration gradient engineering represents an integrative framework that unifies transport regulation, solvation modulation, and interfacial control under the concept of spatially resolved ion distribution, providing a coherent theoretical basis for understanding and designing stable and high-performance aqueous Zn batteries.</p>
    </sec>
    <sec id="sec2">
      <title>GRADIENT ENGINEERING IN LIQUID ELECTROLYTES</title>
      <p>In liquid electrolyte systems, concentration gradient engineering serves as a fundamental strategy for regulating Zn<sup>2+</sup> transport and interfacial reactions, thereby stabilizing Zn electrode behavior. Owing to the high mobility of ions and solvent molecules, liquid electrolytes are particularly sensitive to local concentration fluctuations and interfacial chemistry. By deliberately introducing spatially asymmetric ion distributions, it becomes possible to modulate the Zn<sup>2+</sup> solvation structure, electric double-layer configuration, and ion flux near the electrode surface. In this regard, various approaches have been developed to construct ion concentration gradients in liquid electrolytes, primarily through the use of functional electrolyte additives and ion-selective separators.</p>
      <sec id="sec2-1">
        <title>Functional additive regulation</title>
        <p>In conventional aqueous liquid electrolytes, functional additives enable the construction of Zn<sup>2+</sup> concentration gradients primarily through competitive coordination, interfacial adsorption, and modulation of the electric double layer. Additives containing electron-donating functional groups can partially replace water molecules in the primary solvation sheath of Zn<sup>2+</sup>, thereby reconstructing its solvation structure and altering desolvation kinetics<sup>[<xref ref-type="bibr" rid="B69">69</xref>,<xref ref-type="bibr" rid="B70">70</xref>]</sup>. Owing to their preferential adsorption on the Zn surface, these additives locally increase the amount of coordinated Zn<sup>2+</sup> ions at the electrode and electrolyte interface, generating spatial asymmetry in the chemical potential between the bulk electrolyte and the interfacial region. This gradient drives directional Zn<sup>2+</sup> flux, alleviates ion depletion during plating, and homogenizes nucleation behavior, thereby suppressing dendrite growth and stabilizing interfacial reactions.</p>
        <p>On the basis of this mechanism, Wang <italic>et al.</italic> introduced N, S-doped quantum dots (NSQDs) into the electrolyte to construct a surface Zn<sup>2+</sup> concentration gradient and regulate deposition behavior<sup>[<xref ref-type="bibr" rid="B71">71</xref>]</sup>. The mechanistic basis lies in the abundance of oxygen-containing functional groups located on the side chains of the NSQDs. Upon contact with the Zn foil, these groups undergo partial reduction and anchor onto the metal surface, forming Zn-O bonds<sup>[<xref ref-type="bibr" rid="B72">72</xref>]</sup>. This interfacial chemical coupling creates a Zn<sup>2+</sup>-affinitive layer that is locally enriched with Zn<sup>2+</sup> ions near the electrode, generating a directional ion flux from the bulk electrolyte toward the surface. As a result, numerous uniformly distributed nucleation sites are established, lowering the nucleation overpotential and homogenizing Zn electrodeposition<sup>[<xref ref-type="bibr" rid="B73">73</xref>]</sup>. The formation of this functional interfacial layer was verified by energy dispersive X-ray spectroscopy (EDS) mapping, which revealed uniform distributions of O, N, and S, which were consistent with those of the NSQDs coating, confirming intimate interfacial integration [<xref ref-type="fig" rid="fig2">Figure 2A</xref>]. Owing to the regulated Zn<sup>2+</sup> distribution, the Zn electrode exhibited a significantly smoother and denser morphology after 10 cycles in a symmetric cell at 10 mA cm<sup>-2</sup> with an areal capacity of 0.5 mAh cm<sup>-2</sup>, as evidenced by scanning electron microscopy (SEM) [<xref ref-type="fig" rid="fig2">Figure 2B</xref>]. This interfacial gradient effect is further translated into remarkable full-cell performance. In a Zn-zinc vanadate (ZVO) configuration, the NSQDs-modified system maintained a high specific capacity of <InlineParagraph>208.4 mAh g<sup>-1</sup></InlineParagraph> even at an ultrahigh current density of 10 A g<sup>-1</sup>, substantially outperforming its conventional electrolyte counterpart (44.4 mAh g<sup>-1</sup>). When the current density was restored to 1 A g<sup>-1</sup>, the cell recovered a high capacity of 278.9 mAh g<sup>-1</sup>, demonstrating excellent rate capability and reversibility [<xref ref-type="fig" rid="fig2">Figure 2C</xref>]. These improvements originate from additive-induced interfacial Zn<sup>2+</sup> enrichment and the resulting mitigation of localized ion depletion, which collectively suppress dendrite growth and stabilize the electrochemical reaction environment.</p>
        <fig id="fig2" position="float">
          <label>Figure 2</label>
          <caption>
            <p>(A) SEM image and corresponding EDS mapping of the Zn electrode, which is soaked with the NSQDs dispersion<sup>[<xref ref-type="bibr" rid="B71">71</xref>]</sup>. (B) SEM image after 10 cycles at 10 mA cm<sup>-2</sup> and 0.5 mAh cm<sup>-2</sup> with the NSQDs additive<sup>[<xref ref-type="bibr" rid="B71">71</xref>]</sup>. (C) Rate performance comparison of Zn-ZVO with and without NSQDs<sup>[<xref ref-type="bibr" rid="B71">71</xref>]</sup>. (A-C) Reproduced with permission from<sup>[<xref ref-type="bibr" rid="B71">71</xref>]</sup>. Copyright 2023, Elsevier. (D) Schematic illustration of the DP additive effect at the electrode/electrolyte interface<sup>[<xref ref-type="bibr" rid="B77">77</xref>]</sup>. (E) Operando optical microscopy images of Zn deposition in DP-0 and DP-0.1 electrolytes at 5 mA cm<sup>-2</sup><sup>[<xref ref-type="bibr" rid="B77">77</xref>]</sup>. (F) Rate capability of Zn||NVO full cells with DP-0 and DP-0.1 electrolytes<sup>[<xref ref-type="bibr" rid="B77">77</xref>]</sup>. (D-F) Reproduced with permission from<sup>[<xref ref-type="bibr" rid="B77">77</xref>]</sup>. Copyright 2025, Royal Society of Chemistry.</p>
          </caption>
          <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="em6030.fig.2.jpg" />
        </fig>
        <p>Additive hydrogen bond interactions offer an effective strategy to regulate the Zn electrode interface by restructuring the interfacial water network and tuning Zn<sup>2+</sup> solvation chemistry. In aqueous electrolytes, the hydrogen-bonded network of water governs proton activity, Zn<sup>2+</sup> coordination structure, and interfacial reaction kinetics<sup>[<xref ref-type="bibr" rid="B74">74</xref>]</sup>. The introduction of hydrogen bond-active additives, such as molecules containing hydroxyl, amino, or carbonyl functional groups, enables competitive interactions with water molecules, thereby reducing free water activity and weakening proton transport pathways<sup>[<xref ref-type="bibr" rid="B75">75</xref>,<xref ref-type="bibr" rid="B76">76</xref>]</sup>. This suppression of interfacial water reactivity mitigates the hydrogen evolution reaction and limits the formation of hydroxide byproducts. Simultaneously, the adsorption and interfacial enrichment of such additives reconstruct the electric double layer and modify the Zn<sup>2+</sup> solvation sheath, lowering the desolvation barriers and homogenizing the ion flux. The resulting asymmetric hydrogen-bond environment establishes an ordered interfacial microstructure, which alleviates local ion depletion, stabilizes Zn nucleation, and improves deposition uniformity.</p>
        <p>On the basis of this mechanism, Zong <italic>et al.</italic> introduced diethyl phosphoramidate (DP) as an electrolyte additive to simultaneously regulate hydrogen bonding interactions and Zn<sup>2+</sup> solvation behavior<sup>[<xref ref-type="bibr" rid="B77">77</xref>]</sup>. The polar P=O and N-H functional groups in DP strongly interact with water molecules, disrupting the intrinsic hydrogen bonding network of the aqueous electrolyte and thereby reducing free water activity<sup>[<xref ref-type="bibr" rid="B78">78</xref>]</sup>. This suppression of water reactivity mitigates interfacial pH fluctuations and inhibits parasitic side reactions, particularly the hydrogen evolution reaction. Moreover, DP participates in the Zn<sup>2+</sup> solvation sheath, partially replacing coordinated water molecules and reconstructing the local coordination environment<sup>[<xref ref-type="bibr" rid="B79">79</xref>]</sup>. The modified solvation structure decreases the desolvation energy barrier and accelerates interfacial charge transfer kinetics while simultaneously decreasing the probability of water reduction at the electrode surface. Beyond solvation regulation, DP undergoes interfacial reactions that generate a gradient organic-inorganic hybrid solid electrolyte interphase (SEI) <italic>in situ</italic> [<xref ref-type="fig" rid="fig2">Figure 2D</xref>]. This interphase, enriched with DP-derived species and inorganic Zn compounds, provides abundant and energetically favourable nucleation sites, guiding Zn deposition preferentially along the thermodynamically stable (002) crystallographic plane. The resulting interfacial layer not only homogenizes the electric field distribution but also establishes a more uniform Zn<sup>2+</sup> flux toward the electrode surface, thereby suppressing dendrite formation<sup>[<xref ref-type="bibr" rid="B43">43</xref>]</sup>. <italic>In situ</italic> optical observations at 5 mA cm<sup>-2</sup> clearly reveal this regulatory effect. In the absence of DP, Zn deposition rapidly develops surface protrusions that evolve into dendritic structures, and this behavior indicates severe ion flux heterogeneity. In contrast, the DP-containing electrolyte enables dense and uniform Zn plating throughout the deposition process, and these results confirm that the reconstructed interfacial microenvironment promotes homogeneous nucleation and growth [<xref ref-type="fig" rid="fig2">Figure 2E</xref>]. The interfacial stabilization induced by DP translates directly into enhanced electrochemical performance at the full-cell level. Although cells with and without DP exhibit comparable initial capacities at low current density, the DP-modified system maintains a substantially higher capacity under high-rate conditions and demonstrates excellent reversibility upon returning to lower current densities [<xref ref-type="fig" rid="fig2">Figure 2F</xref>]. These improvements originate from the synergistic effects of hydrogen bond disruption, solvation-structure reconstruction, and gradient SEI formation, which collectively alleviate interfacial side reactions, homogenize Zn<sup>2+</sup> distribution, and stabilize long-term Zn plating/stripping behavior.</p>
      </sec>
      <sec id="sec2-2">
        <title>Ion-selective separator regulation</title>
        <p>In conventional liquid electrolyte systems, ion concentration gradients can be deliberately constructed by introducing functional separators with selective ion transport properties between the anode and cathode. Unlike inert porous membranes that serve only as physical barriers, these engineered separators contain fixed charges, polar functional groups, or well-defined ion-conductive channels that regulate Zn<sup>2+</sup> migration through electrostatic interactions, selective coordination, and Donnan exclusion effects<sup>[<xref ref-type="bibr" rid="B80">80</xref>,<xref ref-type="bibr" rid="B81">81</xref>]</sup>. This selective transport behavior redistributes Zn<sup>2+</sup> flux and creates spatial asymmetry in the ion concentration within the electrolyte region, thereby establishing a controlled chemical potential gradient toward the Zn electrode surface. Moreover, the tailored internal structure of the separator modulates the local electric field distribution and constrains ion diffusion pathways, which alleviates localized ion depletion and suppresses the field amplification that typically drives dendritic growth. In certain systems, solvent transport and water activity near the anode are also regulated, leading to reduced hydrogen evolution and surface passivation. Through the combined effects of ion sieving, electric field homogenization, and mass transport control, functional separators provide an effective platform for stabilizing Zn<sup>2+</sup> flux and improving interfacial deposition behavior.</p>
        <p>On the basis of this design principle, Liu <italic>et al.</italic> developed a bifunctional composite separator (BC-FP) using a nanoconfinement and gradient ion-guiding strategy to regulate Zn<sup>2+</sup> transport and deposition<sup>[<xref ref-type="bibr" rid="B82">82</xref>]</sup>. The separator integrates a bacterial cellulose layer with a filter paper substrate, enabling synergistic control over ion migration and interfacial kinetics. The bacterial cellulose component is rich in zincophilic hydroxyl groups that can coordinate with Zn<sup>2+</sup> ions, thereby reconstructing local transport pathways and stabilizing the interfacial microenvironment by suppressing parasitic side reactions [<xref ref-type="fig" rid="fig3">Figure 3A</xref>]. Moreover, the hydrophilic filter paper layer facilitates directional Zn<sup>2+</sup> transport through capillary-driven electrolyte uptake, promoting a continuous and guided ion flux toward the anode. The intrinsic gradient pore structure across the composite further modulates mass transport by enhancing ion diffusion while preventing localized ion depletion. This structural asymmetry establishes a spatially regulated Zn<sup>2+</sup> concentration profile and homogenizes the desolvation process of hydrated Zn<sup>2+</sup> ions at the electrode surface, leading to uniform nucleation behavior. After cycling a Zn symmetric cell at 1 mA cm<sup>-2</sup> for 30 min, the Zn electrode under BC-FP conditions exhibited a dense and smooth surface morphology, indicating that the Zn deposition stabilized compared with that of conventional separators [<xref ref-type="fig" rid="fig3">Figure 3B</xref>]. In full cells employing a Zn anode and a vanadium-based cathode, the BC-FP separator consistently delivers higher specific capacities across a wide range of current densities than glass fibre separators do. At high rates, the capacity advantage becomes particularly pronounced, and the cell maintains excellent reversibility when the current density is restored to lower values [<xref ref-type="fig" rid="fig3">Figure 3C</xref>].</p>
        <fig id="fig3" position="float">
          <label>Figure 3</label>
          <caption>
            <p>(A) Schematic illustration of the assembled Zn-V<sub>2</sub>O<sub>5</sub> full cell with a 2 M ZnSO<sub>4</sub> electrolyte<sup>[<xref ref-type="bibr" rid="B82">82</xref>]</sup>. (B) SEM image of Zn electrodes after 30 min of cycling at 1 mA cm<sup>-2</sup> with a BC-FP separator<sup>[<xref ref-type="bibr" rid="B82">82</xref>]</sup>. (C) Rate performance of Zn-V<sub>2</sub>O<sub>5</sub> full cells with BC-FP and GF separators from 0.2 to 5 A g<sup>-1</sup><sup>[<xref ref-type="bibr" rid="B82">82</xref>]</sup>. (A-C) Reproduced with permission from<sup>[<xref ref-type="bibr" rid="B82">82</xref>]</sup>. Copyright 2025, Elsevier. (D) Schematic illustration of the Zn-NVO full-cell working mechanism<sup>[<xref ref-type="bibr" rid="B85">85</xref>]</sup>. (E) Contact angle of the gBC separator with corresponding optical images<sup>[<xref ref-type="bibr" rid="B85">85</xref>]</sup>. (F) Rate performance of Zn-NVO full cells with GF, BC, and gBC separators<sup>[<xref ref-type="bibr" rid="B85">85</xref>]</sup>. (D-F) Reproduced with permission from<sup>[<xref ref-type="bibr" rid="B85">85</xref>]</sup>. Copyright 2026, Wiley-VCH GmbH.</p>
          </caption>
          <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="em6030.fig.3.jpg" />
        </fig>
        <p>In addition to directly regulating ion transport, ion concentration gradients can also be engineered by tailoring the interactions between separators and water molecules, thereby indirectly modulating Zn<sup>2+</sup> solvation and interfacial mass transport. In aqueous electrolytes, water not only serves as the solvent but also governs proton activity, hydrogen bonding networks, and the solvation structure of Zn<sup>2+</sup> ions. By introducing separators with strong water affinity, hydrogen bond acceptor or donor groups, or confined hydrophilic nanochannels, the local distribution and mobility of water molecules can be spatially regulated. Such separators can preferentially adsorb or immobilize water within their matrix, effectively reducing free water activity near the Zn electrode and reconstructing the hydrogen bonding network<sup>[<xref ref-type="bibr" rid="B83">83</xref>,<xref ref-type="bibr" rid="B84">84</xref>]</sup>. This confinement alters the primary solvation sheath of Zn<sup>2+</sup>, often decreasing the number of coordinated water molecules and lowering desolvation barriers at the interface. Simultaneously, the asymmetric distribution of water across the separator establishes a gradient in solvent activity and chemical potential, which indirectly drives a more uniform Zn<sup>2+</sup> flux toward the electrode surface. This regulated interfacial microenvironment mitigates pH fluctuations, suppresses hydrogen evolution, and prevents the accumulation of hydroxide byproducts.</p>
        <p>On the basis of this mechanism, Dong <italic>et al.</italic> developed an 18 μm thick cellulose separator with a negatively charged surface and gradient hydrophobicity to regulate the solvent distribution and Zn<sup>2+</sup> transport<sup>[<xref ref-type="bibr" rid="B85">85</xref>]</sup>. The negatively charged functional groups within the separator create an electrostatic shielding effect that repels Cl<sup>-</sup> anions while promoting more uniform Zn<sup>2+</sup> flux through selective ion migration [<xref ref-type="fig" rid="fig3">Figure 3D</xref>]. Moreover, the gradient hydrophobic architecture induces asymmetric wettability across the separator thickness, as evidenced by the distinct water contact angles on the two surfaces, which confirms the establishment of a spatially differentiated solvent environment [<xref ref-type="fig" rid="fig3">Figure 3E</xref>]. This asymmetric solvent distribution results in a stepwise desolvation pathway for hydrated Zn<sup>2+</sup> ions, gradually reducing the number of coordinated water molecules as the ions approach the anode. The resulting localized high-concentration electrolyte environment near the electrode effectively suppresses hydrogen evolution and mitigates interfacial side reactions. Through the combined effects of electrostatic regulation, solvent confinement, and progressive desolvation, the separator homogenizes interfacial Zn<sup>2+</sup> transport and stabilizes deposition behavior. Consequently, compared with control systems lacking gradient structural design, full cells employing this separator exhibit superior rate capability and consistently higher specific capacities across a wide range of current densities, demonstrating that solvent-mediated gradient engineering is an effective strategy for enhancing the interfacial stability and electrochemical performance of AZBs [<xref ref-type="fig" rid="fig3">Figure 3F</xref>].</p>
        <p>Notably, the formation of ion concentration gradients is not merely a secondary consequence of interfacial modification but also serves as a fundamental driving factor governing Zn deposition behavior. While interfacial phenomena such as solid electrolyte interphase formation, surface adsorption, and solvation structure regulation can influence local electrochemical environments, their primary role in many systems is to induce or stabilize spatially nonuniform Zn<sup>2+</sup> distributions. These gradients establish chemical potential differences that directly regulate the ion flux, electric field distribution, and nucleation kinetics at the Zn electrode surface. In this sense, ion concentration gradients represent the underlying physical origin of homogenized Zn<sup>2+</sup> transport and uniform deposition.</p>
        <p>Moreover, it is important to recognize that gradient formation is often intrinsically coupled with other interfacial effects. For example, additive adsorption or SEI formation can simultaneously modify the electric double layer and promote localized Zn<sup>2+</sup> enrichment, while confined polymer networks in hydrogel systems regulate both ion transport and solvent activity<sup>[<xref ref-type="bibr" rid="B86">86</xref>]</sup>. These processes act cooperatively to reinforce gradient stability and amplify its regulatory effect on interfacial reactions. Therefore, rather than being independent or competing mechanisms, ion concentration gradients and interfacial modifications should be understood as synergistically coupled, where gradients provide the primary driving force for Zn<sup>2+</sup> flux regulation, and interfacial effects serve as essential enablers that facilitate and stabilize the gradient structure.</p>
      </sec>
    </sec>
    <sec id="sec3">
      <title>GRADIENT ENGINEERING IN HYDROGEL ELECTROLYTES</title>
      <p>In hydrogel electrolyte systems, concentration gradient engineering offers a versatile and effective pathway for regulating ion transport and stabilizing the Zn electrode interface. Owing to their intrinsic polymer networks and tunable physicochemical properties, hydrogel electrolytes enable spatially resolved control over ion migration, solvation structure, and interfacial water activity, which is difficult to achieve in conventional liquid electrolytes<sup>[<xref ref-type="bibr" rid="B87">87</xref>,<xref ref-type="bibr" rid="B88">88</xref>]</sup>. By rationally designing heterogeneous or asymmetric hydrogel architectures, it becomes possible to construct regulated Zn<sup>2+</sup> concentration fields across the electrolyte, thereby guiding ion flux and interfacial reactions. In this context, various gradient construction strategies, such as network density modulation, functional group distribution, compositional layering, and additive-assisted regulation, have been developed to exploit the unique ion transport behavior of hydrogels.</p>
      <p>It should be clarified that gradient structures are fundamentally distinct from general structural heterogeneity. While heterogeneity refers to irregular or nonuniform distributions of network features without defined spatial control, gradient design involves continuous and directional variation in structure or composition, leading to spatially resolved differences in Zn<sup>2+</sup> concentration<sup>[<xref ref-type="bibr" rid="B89">89</xref>]</sup>. This directional asymmetry establishes a chemical potential gradient that actively guides Zn<sup>2+</sup> transport and regulates ion flux at the electrode interface. Therefore, the key distinction lies in the ability of gradient structures to impose controlled ion transport pathways rather than merely introducing structural nonuniformity.</p>
      <sec id="sec3-1">
        <title>Gradient network architecture</title>
        <p>By designing distinct network structures in different regions of hydrogel electrolytes, ion concentration gradients can be established through spatially differentiated ion transport and solvent confinement behavior. In hydrogel systems, the polymer network governs ion mobility, water distribution, and Zn<sup>2+</sup> solvation structure by controlling pore size, crosslinking density, and the distribution of functional groups. Regions with high crosslinking density or reduced pore size impose stronger confinement effects, lowering ion diffusivity and partially immobilizing water molecules, whereas loosely crosslinked domains provide faster ion migration pathways and higher ionic conductivity. This structural heterogeneity generates differences in Zn<sup>2+</sup> transport kinetics and local chemical potential across the hydrogel, thereby creating a controllable ion concentration gradient<sup>[<xref ref-type="bibr" rid="B89">89</xref>,<xref ref-type="bibr" rid="B90">90</xref>]</sup>. Simultaneously, functional groups embedded within the polymer matrix can selectively coordinate with Zn<sup>2+</sup> or participate in hydrogen bonding with water, further modulating the solvation structure and desolvation dynamics near the electrode interface. As hydrated Zn<sup>2+</sup> ions migrate from bulk-like regions toward more confined domains adjacent to the anode, a progressive desolvation process occurs, leading to localized Zn<sup>2+</sup> enrichment and reduced water activity at the interface. This asymmetric microenvironment homogenizes the ion flux, suppresses hydrogen evolution, and stabilizes Zn nucleation behavior.</p>
        <p>On the basis of this principle, Wang <italic>et al.</italic> developed a gradient network hydrogel electrolyte composed of polyvinyl alcohol (PVA), cellulose nanofibres (CNF), and graphene oxide (GO) to regulate Zn<sup>2+</sup> transport and interfacial kinetics in AZBs<sup>[<xref ref-type="bibr" rid="B91">91</xref>]</sup>. The design integrates a low-density PVA and CNF (PC) layer on the cathode side with a high-density PVA, CNF, and GO (PCG) layer adjacent to the Zn anode, thereby establishing spatially differentiated transport properties within a single electrolyte. The cathode-facing layer contains wider transport channels and a higher water content, which facilitates rapid ion migration and maintains high ionic conductivity [<xref ref-type="fig" rid="fig4">Figure 4A</xref>]. In contrast, the dense interfacial network enriched with carboxyl and hydroxyl groups enhances Zn<sup>2+</sup> coordination and promotes progressive desolvation as ions approach the anode. This confined microenvironment reduces local water activity, suppresses parasitic reactions, and homogenizes Zn<sup>2+</sup> flux at the electrode surface. Simulated Zn<sup>2+</sup> concentration fields confirm that compared with homogeneous hydrogels, the gradient structure results in a more uniform interfacial ion distribution, which is consistent with the proposed mechanism of concentration gradient regulation. The electrochemical benefits are reflected in the rate performance, where cells employing the gradient hydrogel deliver average discharge capacities of 250.6, 236.2, 205.7, 159.3, 125.0, 103.6, 89.7, and 236.5 mAh g<sup>-1</sup> at current densities of 0.15, 0.3, 0.6, 1.2, 1.8, 2.4, 3, and 0.15 A g<sup>-1</sup>, respectively [<xref ref-type="fig" rid="fig4">Figure 4B</xref>]. These values consistently exceed those obtained with hydrogels with homogeneous structures, demonstrating that gradient network engineering effectively regulates Zn<sup>2+</sup> transport, stabilizes interfacial deposition, and enhances overall electrochemical performance.</p>
        <fig id="fig4" position="float">
          <label>Figure 4</label>
          <caption>
            <p>(A) Simulated ionic field distributions in PCG20-PC5 systems based on schematic models<sup>[<xref ref-type="bibr" rid="B91">91</xref>]</sup>. (B) Rate performance of Zn-MnO<sub>2</sub> full cells<sup>[<xref ref-type="bibr" rid="B91">91</xref>]</sup>. (A and B) Reproduced with permission from<sup>[<xref ref-type="bibr" rid="B91">91</xref>]</sup>. Copyright 2025, American Chemical Society. (C) CLSM visualization of the GHNs and HHNs<sup>[<xref ref-type="bibr" rid="B90">90</xref>]</sup>. (D) Chronoamperometry of Zn metal in the GHNs and HHNs at -150 mV overpotential<sup>[<xref ref-type="bibr" rid="B90">90</xref>]</sup>. (E) Rate capabilities of Zn-GHNs-PBA and Zn-HHNs-PBA at 0.1-2 A g<sup>-1</sup> within a 1-2 V operating window<sup>[<xref ref-type="bibr" rid="B90">90</xref>]</sup>. (C-E) Reproduced with permission from<sup>[<xref ref-type="bibr" rid="B90">90</xref>]</sup>. Copyright 2024, Wiley-VCH GmbH.</p>
          </caption>
          <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="em6030.fig.4.jpg" />
        </fig>
        <p>Gradient concentration fields can also be constructed through the formation of chemical bonds between the hydrogel electrolytes and the Zn electrode surface, which creates an interfacially anchored and chemically coupled transport layer. When functional groups within the hydrogel network, such as hydroxyl, carboxyl, amino, or sulfonate groups, form coordination or covalent interactions with surface Zn atoms, a tightly bound interphase is generated that differs structurally and chemically from the bulk gel<sup>[<xref ref-type="bibr" rid="B57">57</xref>,<xref ref-type="bibr" rid="B92">92</xref>]</sup>. Compared with the interior hydrogel matrix, this bonded interfacial region exhibits modified ion mobility, solvent distribution, and coordination environments. Chemical anchoring enhances Zn<sup>2+</sup> affinity at the interface and promotes localized ion enrichment, thereby establishing a spatial gradient in Zn<sup>2+</sup> concentration from the bulk electrolyte toward the electrode surface. Simultaneously, the constrained polymer chains and coordinated functional groups facilitate partial desolvation of hydrated Zn<sup>2+</sup> ions and reduce free water activity in the interfacial zone, which suppresses hydrogen evolution and mitigates surface passivation. Interfacial bonding also stabilizes the electric field distribution and minimizes interfacial impedance fluctuations during repeated plating and stripping. Through the synergistic effects of chemical anchoring, solvation reconstruction, and mass transport modulation, hydrogel-Zn interfacial bonding provides a robust strategy for generating controlled concentration gradients and enhancing Zn deposition uniformity and cycling stability in AZBs.</p>
        <p>On the basis of this concept, Cui <italic>et al.</italic> constructed gradient hydrogel networks via an epitaxial polymerization strategy that enables covalent anchoring of the polymer matrix onto the Zn surface<sup>[<xref ref-type="bibr" rid="B90">90</xref>]</sup>. The resulting networks exhibit an asymmetric distribution of negatively charged groups along the thickness direction, which promotes selective Zn<sup>2+</sup> transport and increases the Zn<sup>2+</sup> transference number to 0.65, markedly higher than that of homogeneous hydrogel networks with identical polymer contents. Confocal laser scanning microscopy (CLSM) revealed that the network density gradually decreased from the Zn side interface toward the bulk region, confirming the well-defined gradient architecture, whereas homogeneous hydrogels displayed uniform density along the Z axis [<xref ref-type="fig" rid="fig4">Figure 4C</xref>]. This structural asymmetry establishes differentiated ion mobility and solvent confinement, where the dense interfacial layer restricts lateral diffusion and regulates Zn<sup>2+</sup> desolvation, while the upper region maintains sufficient ionic conductivity. Chronoamperometric measurements further elucidate the transport mechanism. In homogeneous hydrogels, the continuously increasing current within 400 s indicates two-dimensional diffusion and nonuniform deposition [<xref ref-type="fig" rid="fig4">Figure 4D</xref>]. In contrast, the gradient hydrogel exhibited a stable current plateau after 143 s, characteristic of three-dimensional diffusion, demonstrating that the high-density interfacial network effectively homogenized the Zn<sup>2+</sup> flux and stabilized the nucleation behavior<sup>[<xref ref-type="bibr" rid="B82">82</xref>]</sup>. Notably, the term “stable” used here does not imply a strictly constant current response but rather refers to the relatively reduced fluctuation amplitude and smoother evolution of the current over time. These interfacial transport advantages translate to improved electrochemical performance, with full cells delivering capacities of 67, 60, 53, 48, and 44 mAh g<sup>-1</sup> at current densities of 0.1, 0.2, 0.5, 1, and 2 A g<sup>-1</sup>, respectively, compared with 57, 50, 43, 36, and 30 mAh g<sup>-1</sup> for homogeneous hydrogel systems [<xref ref-type="fig" rid="fig4">Figure 4E</xref>]. The superior rate capability confirms that covalently anchored gradient networks effectively regulate interfacial ion transport and reaction kinetics at the Zn electrode.</p>
      </sec>
      <sec id="sec3-2">
        <title>Asymmetric multilayer designs</title>
        <p>Hydrogel electrolytes possess sufficient mechanical robustness and structural flexibility to enable the lamination of multiple hydrogel layers with distinct physicochemical properties, thereby providing a platform for constructing spatially controlled ion concentration gradients. When hydrogels with different crosslinking densities, pore structures, functional group distributions, or water contents are stacked together, each layer exhibits unique ion transport kinetics, solvent activity, and Zn<sup>2+</sup> coordination behavior. Regions with loose networks and high water content typically offer high ionic conductivity and rapid Zn<sup>2+</sup> migration, whereas densely crosslinked or functionally enriched layers impose stronger confinement effects, reduce water mobility, and enhance Zn<sup>2+</sup> coordination interactions<sup>[<xref ref-type="bibr" rid="B93">93</xref>,<xref ref-type="bibr" rid="B94">94</xref>]</sup>. This structural heterogeneity generates differences in diffusion coefficients and chemical potentials across the electrolyte thickness, resulting in a directional Zn<sup>2+</sup> flux from high-mobility domains toward more confined interfacial regions. As hydrated Zn<sup>2+</sup> ions traverse these layers, progressive desolvation and solvent reorganization occur, leading to localized Zn<sup>2+</sup> enrichment and reduced free water activity near the electrode surface. The resulting asymmetric transport environment homogenizes the interfacial ion distribution, suppresses hydrogen evolution, and stabilizes Zn nucleation and growth. Through the integration of mass transport modulation, solvent confinement, and solvation structure tuning, laminated hydrogel electrolytes enable rational gradient engineering to enhance the interfacial stability and electrochemical performance of AZBs.</p>
        <p>On the basis of this concept, Lu <italic>et al.</italic> proposed a directional electrolyte gradient strategy that establishes a Zn<sup>2+</sup> concentration gradient from the separator toward the anode to simultaneously optimize wettability and interfacial deposition behavior<sup>[<xref ref-type="bibr" rid="B95">95</xref>]</sup>. In this configuration, a high-concentration electrolyte integrated with a sodium carboxymethyl cellulose binder is coated directly onto the Zn surface, while a low-concentration electrolyte fully infiltrates the glass fibre separator [<xref ref-type="fig" rid="fig5">Figure 5A</xref>]. This spatially differentiated design creates distinct physicochemical environments across the cell. The low-concentration region ensures sufficient wettability and facilitates long-range Zn<sup>2+</sup> migration within the separator, whereas the high-concentration region adjacent to the Zn anode promotes dense and uniform Zn deposition by reducing water activity, suppressing parasitic reactions, and stabilizing the interfacial electric field. Optical observations after 10 h of evaporation reveal a gradual transition in light transmittance from top to bottom, which is consistent with an increasing concentration of crystalline hydrated zinc sulfate, confirming the formation of the intended concentration gradient [<xref ref-type="fig" rid="fig5">Figure 5B</xref>]. The distribution of carboxymethyl cellulose particles further supports this gradient structure, with spherical and chain-like aggregates concentrated near the bottom region and flake-like structures observed near the top, reflecting morphology-dependent migration behavior during solvent redistribution. The electrochemical advantages of this gradient design are evident in full cells assembled with Zn anodes and V<sub>2</sub>O<sub>5</sub> cathodes. Under gradient electrolyte conditions, the cell retains a specific capacity of 92 mAh g<sup>-1</sup> after 800 cycles, whereas a cell using a conventional liquid electrolyte decreases to 37 mAh g<sup>-1</sup> after only 200 cycles. The gradient system also exhibits more stable and narrowly distributed Coulombic efficiency, indicating suppressed side reactions and stabilized interfacial kinetics [<xref ref-type="fig" rid="fig5">Figure 5C</xref>]. These results demonstrate that a spatially controlled electrolyte concentration effectively regulates Zn<sup>2+</sup> flux and interfacial reactions, leading to significantly enhanced cycling stability.</p>
        <fig id="fig5" position="float">
          <label>Figure 5</label>
          <caption>
            <p>(A) Schematic of the gradient electrolyte strategy for AZBs<sup>[<xref ref-type="bibr" rid="B95">95</xref>]</sup>. (B) Optical photograph showing the concentration distribution of CMC in the gradient electrolyte<sup>[<xref ref-type="bibr" rid="B95">95</xref>]</sup>. (C) Discharge capacity and Coulombic efficiency of Zn-V<sub>2</sub>O<sub>5</sub> cells with 1 M ZnSO<sub>4</sub> and 1 M@CMC|1 M ZnSO<sub>4</sub> electrolytes at 500 mA g<sup>-1</sup><sup>[<xref ref-type="bibr" rid="B95">95</xref>]</sup>. (A-C) Reproduced with permission from<sup>[<xref ref-type="bibr" rid="B95">95</xref>]</sup>. Copyright 2023, Wiley-VCH GmbH. (D) Cross-section of the AHE<sup>[<xref ref-type="bibr" rid="B96">96</xref>]</sup>. (E) CLSM image of the Zn anode after 100 h in the hydrogel electrolyte<sup>[<xref ref-type="bibr" rid="B96">96</xref>]</sup>. (F) Zn-I<sub>2</sub> full-cell rate performance from 0.1 to <InlineParagraph>10 A g<sup>-1</sup><sup>[<xref ref-type="bibr" rid="B96">96</xref>]</sup>.</InlineParagraph> (D-F) Reproduced with permission from<sup>[<xref ref-type="bibr" rid="B96">96</xref>]</sup>. Copyright 2024, American Chemical Society.</p>
          </caption>
          <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="em6030.fig.5.jpg" />
        </fig>
        <p>Moreover, this gradient electrolyte design strategy can be extended to Zn-I<sub>2</sub> battery systems, where it simultaneously regulates Zn anode stability and iodine redox kinetics through spatially differentiated ionic environments. In Zn-I<sub>2</sub> batteries, performance degradation typically arises from two coupled issues: dendritic Zn deposition at the anode and the dissolution and shuttling of polyiodide species at the cathode<sup>[<xref ref-type="bibr" rid="B96">96</xref>]</sup>. By constructing a Zn<sup>2+</sup> concentration gradient from the separator toward the Zn surface, a high-concentration electrolyte region adjacent to the anode reduces water activity, suppresses hydrogen evolution, and homogenizes Zn<sup>2+</sup> flux, thereby stabilizing Zn plating and stripping. Moreover, maintaining a relatively low concentration environment near the separator and cathode preserves sufficient ionic conductivity and facilitates efficient redox conversion of iodine species<sup>[<xref ref-type="bibr" rid="B97">97</xref>,<xref ref-type="bibr" rid="B98">98</xref>]</sup>. Concentration asymmetry also influences the distribution and diffusion behavior of polyiodide intermediates, as modified solvent activity and ion-pairing interactions can restrict their outwards migration and mitigate shuttle effects. Consequently, the gradient electrolyte establishes a coordinated regulatory mechanism that balances Zn<sup>2+</sup> transport, solvent reactivity, and iodine conversion dynamics.</p>
        <p>On the basis of this principle, Liu <italic>et al.</italic> constructed an asymmetric hydrogel electrolyte to achieve spatially differentiated interfacial regulation in Zn-I<sub>2</sub> batteries<sup>[<xref ref-type="bibr" rid="B96">96</xref>]</sup>. On the anode side, a Zn<sup>2+</sup>-crosslinked sodium alginate and carrageenan double-network hydrogel was employed to guide Zn<sup>2+</sup> transport and stabilize the deposition behavior [<xref ref-type="fig" rid="fig5">Figure 5D</xref>]. The abundant coordination sites within this dense network promote uniform Zn<sup>2+</sup> distribution, facilitate controlled desolvation, and suppress dendritic growth, thereby enabling dendrite-free Zn plating and long-term interfacial stability. On the cathode side, a highly conductive PVA-reinforced poly(3,4-ethylenedioxythiophene) polystyrene hydrogel (PVA-PEDOT) was introduced to immobilize polyiodide intermediates and accelerate electron transfer, effectively mitigating the shuttle effect while enhancing I<sub>2</sub> to I<sup>-</sup> redox kinetics. This asymmetric configuration integrates ion transport regulation at the anode with redox confinement at the cathode, forming a coordinated gradient microenvironment across the cell. After operation at 5 mA cm<sup>-2</sup> for 100 h, the Zn surface remained flat and dense, with a height variation of only 24 μm, confirming highly uniform deposition [<xref ref-type="fig" rid="fig5">Figure 5E</xref>]. The electrochemical advantages are reflected in the rate performance, where the full cell delivers capacities of 210 and 150 mAh g<sup>-1</sup> at 0.1 and <InlineParagraph>10 A g<sup>-1</sup>,</InlineParagraph> respectively, and nearly fully recovers its initial capacity when the current density returns to <InlineParagraph>0.1 A g<sup>-1</sup></InlineParagraph> [<xref ref-type="fig" rid="fig5">Figure 5F</xref>]. Compared with cells using conventional liquid electrolytes, cells using asymmetric hydrogel electrolytes demonstrate markedly improved stability and reversibility, highlighting the effectiveness of spatially engineered hydrogel systems in regulating interfacial reactions and enhancing battery performance.</p>
      </sec>
      <sec id="sec3-3">
        <title>Additive-assisted designs</title>
        <p>Like conventional liquid systems, ion concentration gradients in hydrogel electrolytes can be established through the incorporation of functional additives that synergistically interact with both the polymer network and solvated Zn<sup>2+</sup> species. In hydrogel matrices, ion transport is inherently influenced by network confinement, fixed charges, and solvent distribution. When additives containing coordination groups or hydrogen bond-active moieties are introduced, they can selectively bind Zn<sup>2+</sup> ions or restructure the local water environment, thereby modifying solvation configurations and ion mobility within specific regions of the gel. Because diffusion and segmental motion in hydrogels are spatially heterogeneous, compared with those in additive-free regions, Zn<sup>2+</sup> transport kinetics and chemical potentials in hydrogels in additive-enriched regions often differ<sup>[<xref ref-type="bibr" rid="B58">58</xref>,<xref ref-type="bibr" rid="B99">99</xref>]</sup>. This spatial variation generates a controllable Zn<sup>2+</sup> concentration gradient across the electrolyte thickness. Near the anode interface, additive-induced coordination and solvent confinement promote progressive desolvation, reduce free water activity, and homogenize Zn<sup>2+</sup> flux, whereas the bulk region maintains sufficient ionic conductivity for efficient charge transport. In some systems, additive participation in interfacial reactions further stabilizes the electrode surface by forming a reinforced interphase integrated with the polymer network. Through the combined effects of solvation tuning, selective coordination, and network-dependent mass transport modulation, additive functionalization in hydrogel electrolytes provides a versatile strategy for constructing ion concentration gradients and enhancing interfacial stability in AZBs.</p>
        <p>On the basis of this strategy, Liu <italic>et al.</italic> introduced a zincophilic betaine (BT) additive into a functional hydrogel electrolyte to regulate interfacial chemistry and construct a favourable solid electrolyte interphase<sup>[<xref ref-type="bibr" rid="B100">100</xref>]</sup>. Owing to the robust interfacial contact established by the <italic>in situ</italic> sol-gel transition, BT molecules preferentially adsorb onto the Zn surface through their zinc-affinitive -COO groups, whereas the hydrophobic -CH<sub>3</sub> groups orient toward the electrolyte, thereby reconstructing the electric double layer and inducing the formation of a hybrid SEI with an organic-rich outer layer [<xref ref-type="fig" rid="fig6">Figure 6A</xref>]. This adsorption configuration displaces water molecules from the inner Helmholtz plane and simultaneously suppresses their replenishment from the outer Helmholtz plane, establishing a water-deficient interface that mitigates hydrogen evolution and other parasitic reactions. Compared with its <italic>ex situ</italic>-assembled counterpart, the <italic>in situ</italic>-constructed Zn/gel-BT/Zn symmetric cell exhibits markedly lower interfacial resistance, confirming improved interfacial contact and accelerated Zn<sup>2+</sup> transport [<xref ref-type="fig" rid="fig6">Figure 6B</xref>]. Owing to the regulated SEI formation and homogenized ion flux, the symmetric cell achieves stable cycling for up to 450 h at 5 mA cm<sup>-2</sup> and 10 mAh cm<sup>-2</sup> [<xref ref-type="fig" rid="fig6">Figure 6C</xref>]. In Zn-Cu asymmetric cells, the gel BT electrolyte maintains exceptionally high Coulombic efficiency as the current density increases from 1 to 10 mA cm<sup>-2</sup> and preserves ultrahigh reversibility when the current density is switched back to 1 mA cm<sup>-2</sup>, whereas cells without BT display pronounced efficiency fluctuations under elevated current densities [<xref ref-type="fig" rid="fig6">Figure 6D</xref>]. These results collectively demonstrate that BT-enabled interfacial reconstruction in hydrogel electrolytes effectively suppresses water-induced side reactions and uncontrolled dendrite growth, thereby enhancing the stability and reversibility of Zn plating and stripping.</p>
        <fig id="fig6" position="float" width="550">
          <label>Figure 6</label>
          <caption>
            <p>(A) Schematic of the EDL structure following BT addition<sup>[<xref ref-type="bibr" rid="B100">100</xref>]</sup>. (B) EIS profiles of Zn-Zn cells with <italic>ex situ</italic> and <italic>in situ</italic> gel-BT electrolytes<sup>[<xref ref-type="bibr" rid="B100">100</xref>]</sup>. (C) Cycling performance of Zn symmetrical cells with gel and gel-BT electrolytes at 5 mA cm<sup>-2</sup> and 10 mAh cm<sup>-2</sup><sup>[<xref ref-type="bibr" rid="B100">100</xref>]</sup>. (D) Coulombic efficiency of Zn-Cu cells with gel and gel-BT electrolytes at various current densities<sup>[<xref ref-type="bibr" rid="B100">100</xref>]</sup>. (A-D) Reproduced with permission from<sup>[<xref ref-type="bibr" rid="B100">100</xref>]</sup>. Copyright 2024, Elsevier.</p>
          </caption>
          <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="em6030.fig.6.jpg" />
        </fig>
        <p>From a mechanistic perspective, the solvation and desolvation behavior of Zn<sup>2+</sup> ions plays a critical role in governing interfacial reaction kinetics and deposition morphology. In aqueous electrolytes, Zn<sup>2+</sup> typically exists in a strongly hydrated coordination environment, most commonly forming octahedral [Zn(H<sub>2</sub>O)<sub>6</sub>]<sup>2+</sup> complexes stabilized by hydrogen bonding networks. The desolvation process, which involves partial or complete removal of coordinated water molecules prior to electron transfer, constitutes a key energy barrier that directly influences the nucleation overpotential and charge transfer kinetics at the Zn electrode. This process is highly sensitive to the local coordinated environment and water activity.</p>
        <p>The introduction of ion concentration gradients can indirectly modulate Zn<sup>2+</sup> solvation structures by altering the spatial distribution of ions and solvent molecules near the interface. In regions with elevated Zn<sup>2+</sup> concentrations, the relative availability of free water molecules decreases, leading to reduced water activity and a higher probability of contact ion pairs or solvent-shared ion configurations<sup>[<xref ref-type="bibr" rid="B101">101</xref>]</sup>. This shift in the coordination environment facilitates partial desolvation and decreases the energy barrier for Zn<sup>2+</sup> reduction. Conversely, in bulk-like regions with higher water activity, fully hydrated Zn<sup>2+</sup> species dominate, supporting efficient long-range ion transport. Such spatial variation establishes a progressive desolvation pathway as Zn<sup>2+</sup> ions migrate toward the electrode, coupling ion transport with solvation dynamics.</p>
        <p>Furthermore, water activity not only governs solvation structure but also influences interfacial side reactions, particularly the hydrogen evolution reaction and hydroxide formation. Reduced water activity near the Zn surface suppresses proton reduction and stabilizes the interfacial pH, thereby mitigating parasitic reactions and surface passivation<sup>[<xref ref-type="bibr" rid="B102">102</xref>]</sup>. Therefore, effective gradient engineering should consider not only the Zn<sup>2+</sup> concentration distribution but also the coupled regulation of coordination chemistry and water activity. This integrated perspective provides a more comprehensive understanding of how gradient structures influence interfacial reaction kinetics and highlights the importance of solvation transport coupling in the design of advanced electrolyte systems for AZBs.</p>
      </sec>
      <sec id="sec3-4">
        <title>Advanced characterization techniques and simulation</title>
        <p>In the design of Zn<sup>2+</sup> concentration gradients, advanced characterization techniques combined with quantitative simulation are indispensable for verifying gradient formation and clarifying how spatial Zn<sup>2+</sup> distribution regulates interfacial reactions. Electrochemical measurements such as electrochemical impedance spectroscopy, galvanostatic intermittent titration, chronoamperometry, and transference number tests provide key kinetic parameters, including ionic conductivity, charge transfer resistance, Zn<sup>2+</sup> diffusion coefficients, and Zn<sup>2+</sup> transference numbers. These experimentally derived parameters can be incorporated into continuum-scale models based on the Nernst-Planck and Poisson equations or finite element simulations to quantitatively reconstruct Zn<sup>2+</sup> concentration fields and electric potential distributions across the electrolyte and near the electrode interface<sup>[<xref ref-type="bibr" rid="B103">103</xref>,<xref ref-type="bibr" rid="B104">104</xref>]</sup>. It should be clarified that the above two references support the fundamental governing equations and the general modelling framework for metal electrodeposition rather than a specific electrochemical system. Although these studies focus on Li metal systems, the underlying theoretical descriptions, including ion transport, electric field distribution, and interface evolution, are based on general electrochemical principles that are also applicable to Zn deposition. By correlating simulated ion flux profiles with operando or <italic>ex situ</italic> characterization methods such as <italic>in situ</italic> optical microscopy, CLSM, Raman mapping, X-ray photoelectron spectroscopy depth profiling, and electron microscopy of deposited Zn, directly linking gradient-regulated ion transport behavior with nucleation thermodynamics and growth morphology becomes possible. This integrated strategy, in which electrochemical data serve as input parameters for ion transport modelling and are cross-validated by spatially resolved structural and compositional analyses, enables a mechanistic understanding of how engineered Zn<sup>2+</sup> concentration gradients suppress side reactions, homogenize interfacial current distribution, and stabilize Zn plating and stripping processes.</p>
        <p>On the basis of the above strategy, Cui <italic>et al.</italic> designed a viscosity gradient electrolyte configuration by inserting filter paper to spatially divide the electrolyte into a high-viscosity Zn<sup>2+</sup> ion buffer layer and a low-viscosity bulk transport region, thereby constructing an asymmetric Zn<sup>2+</sup> concentration regulation pathway<sup>[<xref ref-type="bibr" rid="B105">105</xref>]</sup>. In this architecture, the high viscosity region adjacent to the Zn anode retards Zn<sup>2+</sup> migration and alleviates local ion depletion, which homogenizes interfacial Zn<sup>2+</sup> flux and promotes uniform nucleation, whereas the low viscosity region maintains rapid ion transport and low internal resistance. Simulations of Zn<sup>2+</sup> concentration profiles after charging at 5 mA cm<sup>-2</sup> for 720 s reveal that the decrease in Zn<sup>2+</sup> concentration at the cathode surface is nearly identical in both the electrolyte with a Zn<sup>2+</sup> ion buffer layer and the PVA gel electrolyte, indicating that the thin buffer layer can effectively regulate Zn electrodeposition and induce an ordered Zn<sup>2+</sup> flux comparable to that of a full gel system [<xref ref-type="fig" rid="fig7">Figure 7A</xref>]. Moreover, the Zn<sup>2+</sup> concentration near the anode in the buffer layer system remains close to that in the liquid electrolyte, confirming its spatially selective regulation behavior, and the opposite side preserves Zn<sup>2+</sup> conductivity comparable to that of the liquid electrolyte. This asymmetric modulation enables uniform Zn deposition at lower overpotentials and suppresses parasitic reactions. When charged to an areal capacity of 2 mAh cm<sup>-2</sup> at 5 mA cm<sup>-2</sup>, Zn deposited in the liquid electrolyte exhibits severe nonuniformity, and pronounced hydrogen bubble accumulation is observed in the gel electrolyte, whereas the viscosity gradient configuration yields dense and uniform Zn without obvious gas evolution, reflecting a stabilized interfacial environment <InlineParagraph>[<xref ref-type="fig" rid="fig7">Figure 7B</xref>].</InlineParagraph> Quantitative analysis of deposition kinetics reveals that the initial deposition area coefficient <italic>k<sub>a</sub></italic> and the single-step deposition area increase coefficient <italic>k<sub>s</sub></italic> are lower under viscosity gradient conditions, indicating denser and more reversible Zn growth, whereas the initial Zn<sup>2+</sup> accumulation coefficient <italic>k<sub>m</sub></italic> and the hydrogen evolution onset time coefficient <italic>p<sub>h</sub></italic> are greater, suggesting enhanced Zn<sup>2+</sup> retention and reduced water activity at the interface [<xref ref-type="fig" rid="fig7">Figure 7C</xref>]. The smoother evolution of these parameters further confirms that the constructed Zn<sup>2+</sup> concentration gradient effectively regulates interfacial reaction dynamics and improves cycling stability.</p>
        <fig id="fig7" position="float" width="500">
          <label>Figure 7</label>
          <caption>
            <p>(A) The concentration distribution cloud map of Zn<sup>2+</sup> in different electrolytes at 5 mA cm<sup>-2</sup> via numerical simulations<sup>[<xref ref-type="bibr" rid="B105">105</xref>]</sup>. (B) Macroscopic optical observation photographs at 5 mA cm<sup>-2</sup> and 2 mAh cm<sup>-2</sup> in different electrolytes<sup>[<xref ref-type="bibr" rid="B105">105</xref>]</sup>. (C) Variation curves of four important parameters (<italic>k<sub>a</sub></italic>, <italic>k<sub>s</sub></italic>, <italic>k<sub>m</sub></italic>, and <italic>p<sub>h</sub></italic>)<sup>[<xref ref-type="bibr" rid="B105">105</xref>]</sup>. (A-C) Reproduced with permission from<sup>[<xref ref-type="bibr" rid="B105">105</xref>]</sup>. Copyright 2024, KeAi Publishing. (D) Schematic diagram of the observation mechanism using laser scanning confocal microscopy<sup>[<xref ref-type="bibr" rid="B108">108</xref>]</sup>. (E) Fluorescence emission spectra of 1 M ZnSO<sub>4</sub> with 500 μM HPTS in the pH range of 2.64 to 5.25<sup>[<xref ref-type="bibr" rid="B108">108</xref>]</sup>. (F) The pH distribution around the air electrode charging at 0.05 mA cm<sup>-2</sup> obtained by CLSM<sup>[<xref ref-type="bibr" rid="B108">108</xref>]</sup>. (D-F) Reproduced with permission from<sup>[<xref ref-type="bibr" rid="B108">108</xref>]</sup>. Copyright 2024, American Chemical Society.</p>
          </caption>
          <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="em6030.fig.7.jpg" />
        </fig>
        <p>In addition to reconstructing Zn<sup>2+</sup> concentration fields through electrochemically derived kinetic parameters and numerical simulations, fluorescence-based visualization techniques offer a direct and spatially resolved approach to probe ion concentration gradients <italic>in situ</italic>. This strategy relies on fluorescent probes whose emission intensity, wavelength shift, or lifetime are sensitive to the local Zn<sup>2+</sup> concentration or coordination environment. Upon complexation with Zn<sup>2+</sup>, the electronic structure of the fluorophore is altered, leading to quantifiable optical responses that can be calibrated to the Zn<sup>2+</sup> concentration. By integrating such probes into electrolytes or hydrogel matrices and monitoring fluorescence signals via CLSM or operando optical imaging, two-dimensional or three-dimensional maps of Zn<sup>2+</sup> distribution can be constructed across the electrolyte and near the electrode interface<sup>[<xref ref-type="bibr" rid="B106">106</xref>,<xref ref-type="bibr" rid="B107">107</xref>]</sup>. Time-resolved fluorescence imaging further enables the tracking of dynamic concentration evolution during plating and stripping processes, revealing ion depletion, accumulation, and flux heterogeneity under different current densities. When correlated with electrochemical data and modelled ion transport profiles, fluorescence visualization provides complementary validation of gradient formation and clarifies how localized Zn<sup>2+</sup> enrichment or depletion governs nucleation behavior, interfacial stability, and dendrite growth. This combined optical and electrochemical methodology, therefore, establishes a powerful platform for elucidating the mechanistic role of engineered Zn<sup>2+</sup> concentration gradients in AZBs.</p>
        <p>On the basis of the above mechanism, Chen <italic>et al.</italic> introduced CLSM to realize operando visualization of ion transport by coupling fluorescence imaging with electrochemical processes in a neutral Zn air battery model system<sup>[<xref ref-type="bibr" rid="B108">108</xref>]</sup>. A pH-sensitive fluorescent probe was employed to convert local ion transport-induced fluctuations in pH into measurable optical signals, thereby enabling indirect mapping of interfacial ion dynamics [<xref ref-type="fig" rid="fig7">Figure 7D</xref>]. After immersion in the ZnSO<sub>4</sub> electrolyte, pronounced fluctuations in the pH with pulsation behavior were observed near the Zn electrode, reflecting severe hydrogen evolution and periodic variations in reaction intensity, whereas a galvanized Zn electrode exhibited much smaller fluctuations in the pH, indicating improved corrosion resistance and suppressed parasitic reactions. At the air electrode, distinct spatial heterogeneity in ion transport was detected during both discharge and charge, and with increasing current density, the dominant transport mode gradually shifted from diffusion-controlled to convection diffusion-coupled behavior, highlighting the increasing contribution of convection to internal ion migration. To establish a quantitative relationship between the fluorescence response and pH, the emission spectra of an electrolyte containing 1 M ZnSO<sub>4</sub> and 500 μM 8-hydroxypyrene 1,3,6-trisulfonic acid trisodium salt were recorded under 458 nm excitation with emission collected from 480 to 580 nm [<xref ref-type="fig" rid="fig7">Figure 7E</xref>]. The fluorescence intensity increased monotonically with increasing pH and reached a maximum at approximately 510 nm, providing a calibration basis for confocal imaging. On the basis of this correlation, <italic>in situ</italic> imaging during charging revealed that the fluorescence intensity near the electrode decreased within the first 50 to 100 s, indicating a transient local pH decrease caused by the diffusion of alkaline species into the bulk electrolyte [<xref ref-type="fig" rid="fig7">Figure 7F</xref>]. These results demonstrate that fluorescence-based operando microscopy can be used to quantitatively visualize dynamic ion concentration gradients and elucidate interfacial transport mechanisms in Zn-based electrochemical systems.</p>
        <p>Building upon the insights provided by advanced characterization techniques and simulation methods, it becomes possible to move beyond individual case analyses toward a more unified understanding of ion-concentration gradient engineering. By quantitatively resolving Zn<sup>2+</sup> transport behavior, interfacial reaction kinetics, and spatial concentration distributions, these approaches enable direct comparisons across different gradient design strategies<sup>[<xref ref-type="bibr" rid="B109">109</xref>]</sup>. Despite variations in material systems and structural configurations, the underlying regulatory mechanisms can be broadly categorized into ion transport modulation, solvation structure tuning, and interfacial electric field homogenization. For example, additive-based systems primarily influence Zn<sup>2+</sup> coordination environments and electric double layer structures, whereas separator and hydrogel-based systems impose spatial confinement and directional ion pathways, leading to distinct gradient formation modes ranging from interfacial Zn<sup>2+</sup> enrichment to continuous concentration profiles across the electrolyte<sup>[<xref ref-type="bibr" rid="B110">110</xref>]</sup>.</p>
        <p>Importantly, the effectiveness of these strategies can be quantitatively evaluated through key electrochemical and transport parameters extracted from combined experimental and modelling analyses. Metrics such as the Zn<sup>2+</sup> transference number, nucleation overpotential, interfacial resistance, and chronoamperometric response provide direct insight into the ion flux uniformity and interfacial stability<sup>[<xref ref-type="bibr" rid="B111">111</xref>]</sup>. Moreover, performance indicators, including critical current density, Coulombic efficiency, and long-term cycling stability, reflect the practical impact of gradient regulation on suppressing dendrite growth and parasitic reactions. These quantitative descriptors establish a direct link between the gradient structure, ion transport behavior, and electrochemical performance. On the basis of these correlations, effective gradient engineering should simultaneously regulate interfacial Zn<sup>2+</sup> flux while preserving sufficient bulk ionic conductivity, thereby balancing interfacial stability with overall transport efficiency. This integrated understanding, enabled by advanced characterization and simulation, provides general design principles for the rational development of high-performance aqueous Zn-based batteries.</p>
        <p>Despite the significant progress achieved with advanced characterization techniques such as fluorescence imaging and CLSM, several limitations remain that should be carefully considered when experimental results are interpreted. First, the spatial resolution of these techniques is fundamentally constrained by optical diffraction limits, which may hinder accurate probing of the nanoscale ion distribution and interfacial structures. Second, the quantitative reliability of fluorescence-based methods depends strongly on probe calibration, local environmental sensitivity, and potential interference from factors such as pH variation, ionic strength, and probe aggregation, which can introduce uncertainties in correlating signal intensity with actual Zn<sup>2+</sup> concentration. In addition, these techniques typically rely on exogenous probes that may perturb the native electrolyte environment or alter ion transport behavior.</p>
        <p>Furthermore, capturing rapid and transient ion transport processes under practical operating conditions remains challenging because of limitations in temporal resolution and signal acquisition speed. As a result, experimentally observed concentration profiles may represent time-averaged or partially evolved states rather than true instantaneous distributions<sup>[<xref ref-type="bibr" rid="B90">90</xref>]</sup>. To address these challenges, future efforts should focus on integrating high-resolution operando techniques with quantitative calibration strategies and complementary methods such as electrochemical modelling and spectroscopy. Such multimodal approaches are essential for achieving reliable, spatially resolved, and quantitatively accurate characterization of Zn<sup>2+</sup> concentration gradients and interfacial processes in AZBs.</p>
      </sec>
    </sec>
    <sec id="sec4">
      <title>CONCLUSION AND OUTLOOK</title>
      <p>To provide a clearer comparison of representative strategies and facilitate the extraction of general design principles, key studies are summarized in <xref ref-type="table" rid="t1">Table 1</xref>. Despite differences in electrolyte composition and structural design, these approaches consistently rely on spatial regulation of Zn<sup>2+</sup> distribution to control interfacial behavior. This review demonstrates that ion concentration gradient engineering represents a unifying and mechanism-driven strategy for regulating zinc electrode interfacial reactions in aqueous Zn-based batteries (AZBs). Across both liquid and hydrogel electrolyte systems, diverse material designs converge toward a common objective: spatial control of Zn<sup>2+</sup> transport and interfacial ion distribution. In liquid electrolytes, gradients are primarily established through selective ion-additive interactions and ion-selective separators, which reshape Zn<sup>2+</sup> solvation structures and electric double layers. In hydrogel electrolytes, gradient regulation is achieved via heterogeneous polymer networks, asymmetric compositions, covalent anchoring, and additive-assisted confinement, enabling localized control over ion mobility, water activity, and desolvation kinetics. Despite differences in material form, these strategies share several core mechanistic features: (i) buffering Zn<sup>2+</sup> migration to avoid local depletion or accumulation, (ii) homogenizing interfacial Zn<sup>2+</sup> flux to promote uniform nucleation and growth, and (iii) reducing interfacial water activity to suppress parasitic reactions. Importantly, recent advances in advanced characterization techniques, including concentration-field simulations, parameterized electrochemical analysis, and operando fluorescence visualization, have enabled direct observation of Zn<sup>2+</sup> distribution and its temporal evolution, providing compelling evidence that interfacial stability is intrinsically linked to controlled concentration gradients rather than static material properties alone.</p>
      <table-wrap id="t1">
        <label>Table 1</label>
        <caption>
          <p>Zn<sup>2+</sup> concentration gradient regulation methods described in this review</p>
        </caption>
        <table frame="hsides" rules="groups">
          <thead>
            <tr>
              <td style="border-bottom:1;">
                <bold>Strategy type</bold>
              </td>
              <td style="border-bottom:1;">
                <bold>Electrolyte system</bold>
              </td>
              <td style="border-bottom:1;">
                <bold>Gradient construction strategy</bold>
              </td>
              <td style="border-bottom:1;">
                <bold>Dominant mechanism</bold>
              </td>
              <td style="border-bottom:1;">
                <bold>Current density</bold>
              </td>
              <td style="border-bottom:1;">
                <bold>Cycling performance</bold>
              </td>
            </tr>
          </thead>
          <tbody>
            <tr>
              <td>Additive-based (N,S-doped quantum dots, NSQDs)<sup>[<xref ref-type="bibr" rid="B71">71</xref>]</sup></td>
              <td>ZnSO4 + NSQDs</td>
              <td>Interfacial adsorption-induced Zn<sup>2+</sup> enrichment</td>
              <td>Coordination + electric double layer (EDL) regulation</td>
              <td>10 A g<sup>-1</sup></td>
              <td>208.4 mAh g<sup>-1</sup> (<italic>vs</italic>. 44.4 mAh g<sup>-1</sup> baseline); high reversibility</td>
            </tr>
            <tr>
              <td>Additive-based (diethyl phosphoramidate, DP)<sup>[<xref ref-type="bibr" rid="B77">77</xref>]</sup></td>
              <td>ZnSO<sub>4</sub> + DP</td>
              <td>Hydrogen bond modulation + gradient solid electrolyte interphase (SEI) formation</td>
              <td>Solvation reconstruction + reduced water activity</td>
              <td>5 mA cm<sup>-2</sup></td>
              <td>Uniform deposition; improved rate capability</td>
            </tr>
            <tr>
              <td>Functional separator (bacterial cellulose-filter paper, BC-FP)<sup>[<xref ref-type="bibr" rid="B82">82</xref>]</sup></td>
              <td>ZnSO<sub>4</sub> + BC/FP</td>
              <td>Ion-selective transport + gradient pore structure</td>
              <td>Zn<sup>2+</sup> flux homogenization + nanoconfinement</td>
              <td>1 mA cm<sup>-2</sup></td>
              <td>Smooth Zn morphology; enhanced rate performance</td>
            </tr>
            <tr>
              <td>Solvent-regulating separator (gradient hydrophilic cellulose)<sup>[<xref ref-type="bibr" rid="B85">85</xref>]</sup></td>
              <td>ZnSO<sub>4</sub> + modified cellulose separator</td>
              <td>Water distribution gradient</td>
              <td>Solvation tuning + suppressed hydrogen evolution reaction (HER)</td>
              <td>-</td>
              <td>Improved capacity and cycling stability</td>
            </tr>
            <tr>
              <td>Gradient hydrogel (polyvinyl alcohol/cellulose nanofiber/graphene oxide, PVA/CNF/GO)<sup>[<xref ref-type="bibr" rid="B91">91</xref>]</sup></td>
              <td>PVA/CNF/GO hydrogel</td>
              <td>Crosslinking density gradient</td>
              <td>Ion transport regulation + progressive desolvation</td>
              <td>0.15-3 A g<sup>-1</sup></td>
              <td>250.6 → <InlineParagraph>89.7 mAh g<sup>-1</sup>;</InlineParagraph> superior to homogeneous gels</td>
            </tr>
            <tr>
              <td>Gradient hydrogel networks (GHNs) <italic>vs</italic>. homogeneous hydrogel networks (HHNs)<sup>[<xref ref-type="bibr" rid="B90">90</xref>]</sup></td>
              <td>Covalently anchored polymer/Zn</td>
              <td>Epitaxial polymerization + charge density gradient</td>
              <td>Selective ion transport + 3D diffusion</td>
              <td>0.1-2 A g<sup>-1</sup></td>
              <td>67 → 44 mAh g<sup>-1</sup>; higher than HHNs</td>
            </tr>
            <tr>
              <td>Layered concentration-gradient electrolyte (high-concentration electrolyte@carboxymethyl cellulose, HCE@CMC)<sup>[<xref ref-type="bibr" rid="B95">95</xref>]</sup></td>
              <td>HCE@CMC + dilute electrolyte</td>
              <td>Anode-to-separator concentration gradient</td>
              <td>Water activity regulation + Zn<sup>2+</sup> flux control</td>
              <td>-</td>
              <td>92 mAh g<sup>-1</sup> after 800 cycles (<italic>vs</italic>. <InlineParagraph>37 mAh g<sup>-1</sup></InlineParagraph> after 200 cycles)</td>
            </tr>
            <tr>
              <td>Asymmetric hydrogel electrolyte (AHE) for Zn-I<sub>2</sub> batteries<sup>[<xref ref-type="bibr" rid="B96">96</xref>]</sup></td>
              <td>Carra-Zn-Alg + PVA-PEDOT</td>
              <td>Dual-region functional hydrogel</td>
              <td>Zn<sup>2+</sup> transport regulation + polyiodide confinement</td>
              <td>0.1-10 A g<sup>-1</sup></td>
              <td>210 → 150 mAh g<sup>-1</sup>; capacity recovery at low current</td>
            </tr>
            <tr>
              <td>Additive-functionalized hydrogel (betaine, BT)<sup>[<xref ref-type="bibr" rid="B100">100</xref>]</sup></td>
              <td>Hydrogel + BT</td>
              <td>Interfacial adsorption + electric double layer reconstruction</td>
              <td>Hybrid SEI formation + water exclusion</td>
              <td>5 mA cm<sup>-2</sup></td>
              <td>450 h stable cycling; high CE <InlineParagraph>(1-10 mA cm<sup>-2</sup>)</InlineParagraph></td>
            </tr>
            <tr>
              <td>Electrolyte with Zn<sup>2+</sup> ion buffer layer (EZIBL)<sup>[<xref ref-type="bibr" rid="B105">105</xref>]</sup></td>
              <td>High/low viscosity electrolyte</td>
              <td>Viscosity gradient via ion buffer layer</td>
              <td>Flux buffering + diffusion regulation</td>
              <td>5 mA cm<sup>-2</sup></td>
              <td>Uniform deposition; suppressed HER; stable cycling</td>
            </tr>
          </tbody>
        </table>
	</table-wrap>
      <p>Although significant progress has been made in ion concentration gradient engineering, several key challenges must still be addressed to fully realize its practical potential in AZBs. First, most reported gradient structures are intrinsically static, whereas Zn deposition and stripping involve highly dynamic processes accompanied by the continuous evolution of local electric fields, ion flux, and interfacial chemistry during prolonged cycling and at high current densities. The development of self-adaptive or dynamically regulated gradient systems that can maintain stable ion distributions under realistic operating conditions is therefore important. Second, the lack of quantitative and real-time characterization of local Zn<sup>2+</sup> concentration, water activity, and interfacial chemical states limits the establishment of definitive structure-function relationships. Future studies should integrate advanced operando characterization techniques with electrochemical parameter extraction and numerical modelling to quantitatively correlate ion transport behavior with interfacial reaction mechanisms. Third, a fundamental trade-off remains between interfacial ion regulation and bulk ion transport efficiency. While highly restrictive gradients may suppress dendrite growth, they can also introduce concentration polarization, whereas highly conductive systems may weaken gradient regulation effects. Rational design strategies that spatially decouple bulk ion transport from interfacial ion modulation will therefore be crucial for optimizing both reaction kinetics and mass transport. Finally, many currently reported gradient electrolyte systems rely on complex architectures or sophisticated fabrication processes, which may hinder scalability and practical deployment. Future efforts should thus emphasize simplified and scalable fabrication strategies and evaluate battery performance under practical conditions, including high areal capacities and lean electrolyte configurations.</p>
      <p>Ultimately, ion concentration gradient engineering should be viewed not as a material optimization problem alone but as a spatiotemporal regulation strategy for electrochemical interfaces. By combining rational gradient design with advanced characterization and dynamic regulation concepts, future research can bridge the gap between mechanistic understanding and practical deployment, accelerating the development of durable, high-rate, and commercially viable AZBs.</p>
    </sec>
  </body>
   <back>
    <sec>
      <title>DECLARATIONS</title>
      <sec>
        <title>Author contributions</title>
        <p>Conceptualization, funding acquisition, supervision, writing-review &amp; editing: Cui, Y.</p>
        <p>Investigation: Jin, Z.; Yu, X.</p>
        <p>Supervision, writing-review &amp; editing: He, Y.</p>
        <p>Supervision, project administration, review &amp; editing: Yang, X.</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>Conflicts of interest</title>
        <p>All authors declared that there are no conflicts of interest.</p>
      </sec>
      <sec>
        <title>Financial support and sponsorship</title>
        <p>The authors are thankful for the funding support from the Talent Project of Hefei University (25RC36).</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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