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  <front>
    <journal-meta>
      <journal-id journal-id-type="nlm-ta">AI Agent</journal-id>
      <journal-id journal-id-type="publisher-id">aiagent</journal-id>
      <journal-title-group>
        <journal-title>AI Agent</journal-title>
      </journal-title-group>
      <issn pub-type="epub">3070-3719</issn>
      <publisher>
        <publisher-name>OAE Publishing Inc.</publisher-name>
      </publisher>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.20517/aiagent.2026.21</article-id>
      <article-id pub-id-type="publisher-id">AIAgent-2026-21</article-id>
      <article-categories>
        <subj-group>
          <subject>Perspective</subject>
        </subj-group>
      </article-categories>
      <title-group>
        <article-title>Generative AI for atomistic nanomaterial reconstruction: from static structures to conditioned ensembles</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <name>
            <surname>Liang</surname>
            <given-names>Kairui</given-names>
          </name>
        </contrib>
        <contrib contrib-type="author" corresp="yes">
          <contrib-id contrib-id-type="orcid">https://orcid.org/0009-0003-2325-7538</contrib-id>
          <name>
            <surname>Li</surname>
            <given-names>Xiao-Yan</given-names>
          </name>
          <xref ref-type="corresp" rid="cor1">*</xref>
        </contrib>
      </contrib-group>
      <aff id="I1000">Department of Chemistry, National University of Singapore, Singapore 117543, Singapore.</aff>
      <author-notes>
        <corresp id="cor1">Correspondence to: Asst. Prof. Xiao-Yan Li, Department of Chemistry, National University of Singapore, Singapore 117543, Singapore. E-mail: <email>xiaoyanli@nus.edu.sg</email></corresp>
        <fn fn-type="other">
          <p><bold>Received:</bold> 2 Jun 2026 | <bold>First Decision:</bold> 28 Jul 2026 | <bold>Revised:</bold> 30 Aug 2026 | <bold>Accepted:</bold> 8 Sep 2026 | <bold>Published:</bold> 16 Sep 2026</p>
        </fn>
        <fn fn-type="other">
          <p><bold>Academic Editor:</bold> Aloysius Soon | <bold>Copy Editor:</bold> Tong Wang | <bold>Production Editor:</bold> Tong Wang</p>
        </fn>
      </author-notes>
      <pub-date pub-type="ppub">
        <year>2026</year>
      </pub-date>
      <pub-date pub-type="epub">
        <day>16</day>
        <month>9</month>
        <year>2026</year>
      </pub-date>
      <volume>2</volume>
	  <issue>3</issue>
      <elocation-id>22</elocation-id>
      <permissions>
        <copyright-statement>© The Author(s) 2026.</copyright-statement>
        <license xlink:href="https://creativecommons.org/licenses/by/4.0/">
          <license-p>© The Author(s) 2026.<bold>Open Access</bold>This article is licensed under a Creative Commons Attribution 4.0 International License (<uri xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</uri>), which permits unrestricted use, sharing, adaptation, distribution and reproduction in any medium or format, for any purpose, even commercially, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.</license-p>
        </license>
      </permissions>
    </article-meta>
  </front>
  <body>
    <sec id="sec1">
      <title>INTRODUCTION</title>
      <p>As structure-property relationships in functional nanomaterials have been widely explored<sup>[<xref ref-type="bibr" rid="B1">1</xref>,<xref ref-type="bibr" rid="B2">2</xref>]</sup>, a common strategy is to identify the representative geometric structure that best explains observed material properties<sup>[<xref ref-type="bibr" rid="B3">3</xref>-<xref ref-type="bibr" rid="B5">5</xref>]</sup>. This focus has generally motivated the identification of ground-state or low-energy structures<sup>[<xref ref-type="bibr" rid="B2">2</xref>,<xref ref-type="bibr" rid="B6">6</xref>-<xref ref-type="bibr" rid="B8">8</xref>]</sup>. However, this paradigm does not fully capture the behavior of nanomaterials under realistic operating conditions. Nanomaterial surfaces and interfaces may continuously restructure in response to adsorbates<sup>[<xref ref-type="bibr" rid="B9">9</xref>,<xref ref-type="bibr" rid="B10">10</xref>]</sup>, electrolyte environments<sup>[<xref ref-type="bibr" rid="B11">11</xref>]</sup>, temperature<sup>[<xref ref-type="bibr" rid="B12">12</xref>]</sup>, support interactions<sup>[<xref ref-type="bibr" rid="B13">13</xref>]</sup>, and electrochemical potentials<sup>[<xref ref-type="bibr" rid="B14">14</xref>]</sup>. Here, we use “reconstruction” to refer to such atomistic rearrangement under operating conditions. As a result, experimentally measured behavior often cannot be attributed to a single stable configuration but instead reflects contributions from condition-dependent ensembles of microstates.</p>
      <p>The dynamic structural ensemble reframes the central question in nanomaterial reconstruction studies. The focus therefore shifts from a single stable structure to understanding how accessible states interconvert under operating conditions<sup>[<xref ref-type="bibr" rid="B15">15</xref>,<xref ref-type="bibr" rid="B16">16</xref>]</sup>. Operando characterization provides essential information, but the measured signals are often indirect, time-averaged, making atomic-scale evolution difficult to interpret. For computational modeling, the challenge lies in identifying relevant structures within a vast and unknown configurational space that remains costly to explore at the first-principles level<sup>[<xref ref-type="bibr" rid="B17">17</xref>]</sup>. Therefore, a practical approach should efficiently generate structures, sample metastable microstates, and validate structural distributions under realistic conditions<sup>[<xref ref-type="bibr" rid="B18">18</xref>]</sup>.</p>
      <p>Recent advances in artificial intelligence (AI) and machine learning (ML) are opening new routes for exploring nanomaterial reconstruction. Generative models can learn structural patterns, propose candidate configurations, and sample complex distributions under physical, chemical, or experimental constraints<sup>[<xref ref-type="bibr" rid="B19">19</xref>-<xref ref-type="bibr" rid="B22">22</xref>]</sup>. Related advances in AI-assisted structure generation, multiscale materials modeling, dynamic electrocatalyst simulations, generative materials design, and AI-Agent workflows<sup>[<xref ref-type="bibr" rid="B23">23</xref>-<xref ref-type="bibr" rid="B28">28</xref>]</sup> further motivate integrated approaches to nanomaterial reconstruction.</p>
      <p>In this Perspective, we consider reconstruction as an ensemble problem rather than the identification of a single representative structure. We discuss how generative models, combined with machine learning interatomic potentials (MLIPs), density functional theory (DFT), and operando measurements, can be used to explore dynamic structural ensembles under operating conditions. We further highlight the challenges in sampling, validation, and integration with experiment. Finally, we outline future opportunities for developing more reliable and physically grounded reconstruction workflows.</p>
    </sec>
    <sec id="sec2">
      <title>RECONSTRUCTION AS A STRUCTURE-GENERATION AND ENSEMBLE-INFERENCE PROBLEM</title>
      <p>Nanomaterial surfaces under operating conditions cannot be fully represented by a single stable structure, as atomic rearrangements or even surface atom dissolution may cause multiple interconverting microstates<sup>[<xref ref-type="bibr" rid="B29">29</xref>-<xref ref-type="bibr" rid="B31">31</xref>]</sup>. These microstates differ in defect structures, adsorption configurations, and local coordination environments. Their relative populations depend on different operating conditions<sup>[<xref ref-type="bibr" rid="B3">3</xref>,<xref ref-type="bibr" rid="B10">10</xref>,<xref ref-type="bibr" rid="B30">30</xref>,<xref ref-type="bibr" rid="B32">32</xref>]</sup>.</p>
      <p>For example, Pt nanoparticles retain a clean surface under vacuum [<xref ref-type="fig" rid="fig1">Figure 1A</xref>], whereas CO adsorption induces high-index facets and the formation of new surface layers under CO conditions [<xref ref-type="fig" rid="fig1">Figure 1B</xref>]. Li <italic>et al.</italic> further theoretically revealed that even when Pt nanoparticles reach a dynamic structural equilibrium under CO conditions, their surfaces continue to undergo local structural fluctuations, including the transient formation and dispersion of small clusters [<xref ref-type="fig" rid="fig2">Figure 2</xref>]<sup>[<xref ref-type="bibr" rid="B15">15</xref>]</sup>. These local structural changes are accompanied by fluctuations in catalytic activity, showing that the observed activity reflects an evolving structural ensemble rather than a single static morphology.</p>
      <fig id="fig1" position="float">
        <label>Figure 1</label>
        <caption>
          <p>Adsorbate-induced restructuring example: structural models of a 9.2-nm Pt nanoparticle under vacuum and CO conditions<sup>[<xref ref-type="bibr" rid="B33">33</xref>]</sup>. (A and B) Reprinted with permission from reference<sup>[<xref ref-type="bibr" rid="B33">33</xref>]</sup>. Copyright © 2017 American Chemical Society.</p>
        </caption>
        <graphic xlink:href="aiagent2021.fig.1.jpg"/>
      </fig>
      <fig id="fig2" position="float">
        <label>Figure 2</label>
        <caption>
          <p>Dynamic surface reconstruction and catalytic-activity fluctuations of Pt nanoparticles during CO oxidation<sup>[<xref ref-type="bibr" rid="B15">15</xref>]</sup>. Reprinted with permission from reference<sup>[<xref ref-type="bibr" rid="B15">15</xref>]</sup>, under the terms of the CC BY-NC-ND 4.0 License. TOF: Turnover frequency; NP: nanoparticle.</p>
        </caption>
        <graphic xlink:href="aiagent2021.fig.2.jpg"/>
      </fig>
      <p>Theoretical reconstruction modeling can therefore be formulated as the inference of conditional probability distributions over metastable structures under operating conditions. The structural distribution can be described by <italic>P</italic>(X|<italic>c</italic>), where <italic>c</italic> denotes the relevant external conditions, such as temperature, pressure, electrode potential, pH, and others. Dynamic processes such as activation, deactivation, or phase transitions additionally require a distribution <italic>P</italic>(<italic>τ</italic>|<italic>c</italic>) over reconstruction pathways<sup>[<xref ref-type="bibr" rid="B28">28</xref>,<xref ref-type="bibr" rid="B34">34</xref>]</sup>.</p>
    </sec>
    <sec id="sec3">
      <title>A GENERATIVE-MODEL-BASED WORKFLOW FOR RECONSTRUCTION ENSEMBLE PREDICTION</title>
      <p>We summarize the common generative model-based workflow integrating generative models, MLIPs, and DFT/ab initio molecular dynamics (AIMD) for reconstruction studies through three coupled functions: candidate generation, accelerated sampling, and validation. Generative models broaden the structural search space under operating conditions<sup>[<xref ref-type="bibr" rid="B35">35</xref>,<xref ref-type="bibr" rid="B36">36</xref>]</sup>. MLIPs enable efficient sampling and high-throughput calculations<sup>[<xref ref-type="bibr" rid="B18">18</xref>,<xref ref-type="bibr" rid="B37">37</xref>]</sup>. DFT/AIMD together with experimental constraints can refine and validate representative structures. This generate-accelerate-validate loop in <xref ref-type="fig" rid="fig3">Figure 3</xref> delivers sets of (quasi-)steady-state structures rather than a single optimal configuration. <xref ref-type="table" rid="t1">Table 1</xref> summarizes the main technical approaches discussed in this Perspective and their limitations.</p>
      <fig id="fig3" position="float">
        <label>Figure 3</label>
        <caption>
          <p>Generate-accelerate-validate workflow for nanomaterial reconstruction under operating conditions. Generative models propose condition-dependent candidate structures, MLIPs accelerate configurational sampling, and DFT/AIMD together with experimental observations validate and refine the structural ensemble. The validated information is fed back to improve subsequent sampling and ensemble inference through active learning. AI: Artificial intelligence; MLIPs: machine learning interatomic potentials; DFT: density functional theory; AIMD: ab initio molecular dynamics.</p>
        </caption>
        <graphic xlink:href="aiagent2021.fig.3.jpg"/>
      </fig>
      <table-wrap id="t1">
        <label>Table 1</label>
        <caption>
          <p>Generative and statistical approaches for ensemble modeling</p>
        </caption>
        <table frame="hsides" rules="groups">
  <tbody>
    <tr>
      <td>
        <bold>Approach</bold>
      </td>
      <td>
        <bold>Treatment of physical probabilities</bold>
      </td>
      <td>
        <bold>Main limitation</bold>
      </td>
    </tr>
    <tr>
      <td>Diffusion models<sup>[<xref ref-type="bibr" rid="B38">38</xref>-<xref ref-type="bibr" rid="B40">40</xref>]</sup></td>
      <td>Proposal distribution only; requires reweighting</td>
      <td>Data bias; invalid or unstable candidates</td>
    </tr>
    <tr>
      <td>GFlowNets<sup>[<xref ref-type="bibr" rid="B41">41</xref>,<xref ref-type="bibr" rid="B42">42</xref>]</sup></td>
      <td>Sampling reward; no transition rates</td>
      <td>Trajectories are not physical dynamics</td>
    </tr>
    <tr>
      <td>Boltzmann generators<sup>[<xref ref-type="bibr" rid="B43">43</xref>]</sup></td>
      <td>Explicit equilibrium populations via importance weights</td>
      <td>Needs reliable energy model</td>
    </tr>
    <tr>
      <td>Bayesian reweighting<sup>[<xref ref-type="bibr" rid="B44">44</xref>,<xref ref-type="bibr" rid="B45">45</xref>]</sup></td>
      <td>Experimental-data-constrained update of prior ensemble weights</td>
      <td>Limited by initial ensemble completeness</td>
    </tr>
    <tr>
      <td>MLIP<sup>[<xref ref-type="bibr" rid="B18">18</xref>,<xref ref-type="bibr" rid="B37">37</xref>]</sup></td>
      <td>Enables extended MD and rare-event sampling with near-DFT accuracy</td>
      <td>DFT budget; transferability</td>
    </tr>
    <tr>
      <td>Enhanced sampling<sup>[<xref ref-type="bibr" rid="B18">18</xref>]</sup></td>
      <td>Enhanced free-energy landscapes; reweighting for statistical weights</td>
      <td>CV/bias design; computational cost</td>
    </tr>
  </tbody>
</table>
        <table-wrap-foot>
          <fn id="t1FN1">
            <p>MLIP: Machine learning interatomic potential; DFT: density functional theory; MD: molecular dynamics; CV: collective variable.</p>
          </fn>
        </table-wrap-foot>
      </table-wrap>
      <sec id="sec3-1">
        <title>Stage I - generate &amp; cover</title>
        <p>A conditional generative model can be used to build a diverse pool of physically plausible structures, such as compositions, lattice parameters, defects, or adsorbate patterns. MatterGen provides one concrete example of conditional structure generation under chemical, symmetry, and property constraints<sup>[<xref ref-type="bibr" rid="B46">46</xref>]</sup>. This diffusion-based model was applied to inorganic material design, where experimental validation of one MatterGen-designed material demonstrated a measured property within 20% of the intended target. However, MatterGen was developed primarily for periodic bulk crystals, whereas nanomaterial reconstruction often involves finite particles, variable atom numbers, adsorbate coverages, or grand-canonical composition exchange with the environment. These features are not explicitly represented in conventional bulk-crystal generation benchmarks and must therefore be explicitly considered in surface/interface reconstruction.</p>
      </sec>
      <sec id="sec3-2">
        <title>Stage II - acceleration</title>
        <p>MLIPs extend configurational sampling beyond the time and space scales accessible to direct first-principles calculations. Combined with molecular dynamics, enhanced sampling<sup>[<xref ref-type="bibr" rid="B18">18</xref>]</sup>, or grand-canonical sampling<sup>[<xref ref-type="bibr" rid="B34">34</xref>,<xref ref-type="bibr" rid="B47">47</xref>]</sup>, MLIPs enable broader exploration of accessible microstates. For example, Perego and Bonati proposed a data-efficient active learning scheme (DEAL) using an augmented sampling process for ammonia decomposition on Fe-Co alloy surfaces<sup>[<xref ref-type="bibr" rid="B18">18</xref>]</sup>. Here, configurations with high uncertainty were selectively labeled by DFT and added to the training set. The resulting reactive MLIPs were then used to accelerate reaction-path exploration and kinetic sampling.</p>
      </sec>
      <sec id="sec3-3">
        <title>Stage III - validate &amp; correct</title>
        <p>Representative structures are refined with DFT/AIMD to improve the predicted energetics, barriers, and derived observables. The resulting information can be fed back to update the MLIP and guide subsequent sampling. For example, Wang <italic>et al.</italic> developed a multiscale framework combining grand-canonical Monte Carlo, neural-network molecular dynamics, and first-principles microkinetic modeling to resolve catalyst restructuring at the atomic scale<sup>[<xref ref-type="bibr" rid="B34">34</xref>]</sup>. Beyond first-principles refinement, experimental validation is essential, but operando measurements typically provide indirect, ensemble-averaged signals<sup>[<xref ref-type="bibr" rid="B29">29</xref>]</sup>. Relevant observables, such as X-ray absorption near-edge structure/extended X-ray absorption fine structure (XANES/EXAFS) spectra<sup>[<xref ref-type="bibr" rid="B29">29</xref>]</sup>, pair distribution functions, or microscopy images<sup>[<xref ref-type="bibr" rid="B48">48</xref>]</sup>, provide experimental constraints on the structural ensemble. Corresponding signals can be simulated for candidate structures and combined according to the current ensemble weights. Comparison with experiments can then be used to update these weights through Bayesian or maximum-entropy reweighting<sup>[<xref ref-type="bibr" rid="B44">44</xref>,<xref ref-type="bibr" rid="B45">45</xref>]</sup>, while considering uncertainties in both the calculated and measured signals.</p>
      </sec>
    </sec>
    <sec id="sec4">
      <title>TECHNICAL APPROACHES FOR GENERATIVE AI IN ENSEMBLE MODELING</title>
      <p>After formulating reconstruction as the inference of a conditional structural distribution <italic>P</italic>(X|<italic>c</italic>), the practical challenge is to generate plausible structures under given operating conditions, infer their relative populations, and identify possible reconstruction pathways. Generative AI can contribute to these targets through structure generation, probabilistic ensemble inference, and sequence-based pathway exploration, as summarized in <xref ref-type="fig" rid="fig4">Figure 4A</xref>. <xref ref-type="fig" rid="fig4">Figure 4B</xref> schematically shows two representative generative schemes<sup>[<xref ref-type="bibr" rid="B38">38</xref>-<xref ref-type="bibr" rid="B40">40</xref>,<xref ref-type="bibr" rid="B43">43</xref>]</sup>. Diffusion-based models progressively add noise to an initial structure x<sub>0</sub> through a fixed forward Markov chain and generate candidate structures through a learned reverse denoising process (indicated by dashed arrows)<sup>[<xref ref-type="bibr" rid="B38">38</xref>-<xref ref-type="bibr" rid="B40">40</xref>,<xref ref-type="bibr" rid="B43">43</xref>]</sup>.</p>
      <fig id="fig4" position="float">
        <label>Figure 4</label>
        <caption>
          <p>Roles of generative AI in nanomaterial reconstruction. (A) Conceptual roles of generative AI, including candidate structure generation, probabilistic ensemble inference, and reconstruction-pathway sampling; (B) Representative flow-based and diffusion-based generative schemes for structure generation. Flow-based models learn transformations between structural and latent representations<sup>[<xref ref-type="bibr" rid="B38">38</xref>-<xref ref-type="bibr" rid="B40">40</xref>,<xref ref-type="bibr" rid="B43">43</xref>]</sup>. Diffusion models progressively perturb structures with noise and learn a reverse denoising process to generate candidate structures<sup>[<xref ref-type="bibr" rid="B38">38</xref>-<xref ref-type="bibr" rid="B40">40</xref>,<xref ref-type="bibr" rid="B43">43</xref>]</sup>. AI: Artificial intelligence.</p>
        </caption>
        <graphic xlink:href="aiagent2021.fig.4.jpg"/>
      </fig>
      <sec id="sec4-1">
        <title>Structure generation with diffusion models</title>
        <p>E(3)-equivariant diffusion models provide a framework for atomic structure generation by considering geometric symmetry of three-dimensional space during the denoising process<sup>[<xref ref-type="bibr" rid="B38">38</xref>]</sup>. Diffusion models have also been extended to jointly generate lattice parameters and atomic coordinates<sup>[<xref ref-type="bibr" rid="B39">39</xref>]</sup>. However, unconstrained generation can produce structures with little physical relevance<sup>[<xref ref-type="bibr" rid="B26">26</xref>,<xref ref-type="bibr" rid="B49">49</xref>]</sup>, motivating the incorporation of physical priors and experimental constraints. Rønne <italic>et al.</italic> developed a diffusion model specifically for surface structure discovery by introducing substrate coordination and confinement along the surface-normal direction<sup>[<xref ref-type="bibr" rid="B40">40</xref>]</sup>. This work demonstrates how diffusion models can be adapted from periodic bulk crystals to surface reconstruction and condition-dependent structural exploration.</p>
      </sec>
      <sec id="sec4-2">
        <title>Probabilistic ensemble inference</title>
        <p>Probabilistic ensemble inference aims to estimate structural distributions and relative populations under specified operating conditions. Within this framework, ensemble reweighting uses experimental measurements to update the statistical weights assigned to an initial set of candidate structures. Boltzmann generators can facilitate sampling of thermodynamic ensembles<sup>[<xref ref-type="bibr" rid="B43">43</xref>]</sup>, whereas Bayesian maximum-entropy methods can update the weights of candidate structures using experimental constraints<sup>[<xref ref-type="bibr" rid="B44">44</xref>]</sup>. Notably, reweighting can only redistribute the populations among structures already included in the candidate set. Therefore, generative models can be used beforehand to broaden the candidate set and improve the coverage of experimentally relevant structures.</p>
      </sec>
      <sec id="sec4-3">
        <title>Sequence-based pathway exploration</title>
        <p>Sequence-based generative models such as Generative Flow Networks (GFlowNets)<sup>[<xref ref-type="bibr" rid="B41">41</xref>]</sup> build structures step by step and sample multiple candidates according to a defined reward. For example, Crystal-GFlowNet sequentially samples crystal structures under compositional and geometric constraints, using rewards (e.g., low formation energy) to explore a broad range of candidate structures<sup>[<xref ref-type="bibr" rid="B41">41</xref>,<xref ref-type="bibr" rid="B42">42</xref>]</sup>. For nanomaterial reconstruction, this strategy could be useful for exploring metastable states and proposing possible connections between them. However, trajectories generated by sequence-based generative models are not physical dynamical pathways and therefore do not directly provide transition barriers or rates. Candidate states and transitions proposed by these generative models must be further evaluated using physics-based pathway calculations (e.g., nudged-elastic-band calculations<sup>[<xref ref-type="bibr" rid="B50">50</xref>]</sup>), enhanced-sampling methods<sup>[<xref ref-type="bibr" rid="B18">18</xref>]</sup>, and subsequent kinetic modeling.</p>
      </sec>
    </sec>
    <sec id="sec5">
      <title>OUTLOOK</title>
      <p>Overall, future efforts on atomic-scale reconstruction of nanomaterial surfaces and interfaces should move beyond isolated structure screening toward condition-dependent structural ensembles and reconstruction pathways<sup>[<xref ref-type="bibr" rid="B29">29</xref>,<xref ref-type="bibr" rid="B51">51</xref>,<xref ref-type="bibr" rid="B52">52</xref>]</sup>, together with explicit uncertainty quantification. A central challenge is to represent operating conditions in a physically meaningful way. Temperature, pressure, chemical potential, solvent, electric-double-layer effects, and other external factors should be incorporated through physically appropriate representations or constraints. Such physics-grounded conditioning is critical for transferable ensemble prediction.</p>
      <p>A practical route forward is to integrate conditional generative models<sup>[<xref ref-type="bibr" rid="B46">46</xref>]</sup> with MLIP-accelerated dynamics<sup>[<xref ref-type="bibr" rid="B18">18</xref>,<xref ref-type="bibr" rid="B37">37</xref>]</sup>, first-principles and experimental validation<sup>[<xref ref-type="bibr" rid="B29">29</xref>,<xref ref-type="bibr" rid="B48">48</xref>]</sup>, and uncertainty-aware ensemble reweighting<sup>[<xref ref-type="bibr" rid="B44">44</xref>,<xref ref-type="bibr" rid="B45">45</xref>]</sup>. Within this framework, agents based on large language models (LLMs) can integrate prior knowledge of nanomaterial design from the literature<sup>[<xref ref-type="bibr" rid="B27">27</xref>]</sup>, while multimodal models can integrate heterogeneous structural and chemical representations<sup>[<xref ref-type="bibr" rid="B53">53</xref>]</sup>. Such agentic and multimodal systems can therefore serve as an orchestration and information-integration layer for physics-grounded structure generation and validation.</p>
      <p>Current AI-assisted approaches to studying nanomaterial reconstruction still suffer from limited and biased training data, incomplete sampling of slow reconstruction processes, difficulty in simultaneously incorporating multiple physical and experimental constraints, and limited interpretability. Addressing these issues will require closer integration of thermodynamics, kinetics, and uncertainty quantification. Ultimately, the goal is not only to generate plausible nanostructures, but also to obtain evidence-consistent ensemble predictions that explain how nanomaterials restructure under realistic conditions and how such restructuring controls their functional properties.</p>
    </sec>
  </body>
  <back>
    <sec>
      <title>DECLARATIONS</title>
      <sec>
        <title>Authors’ contributions</title>
        <p>Analyzed and interpreted the literature, prepared figures, and drafted the manuscript: Liang, K.</p>
        <p>Conceived the review scope, provided supervision, revised the manuscript, and guided the overall structure: Li, X. Y.</p>
      </sec>
      <sec>
        <title>Availability of data and materials</title>
        <p>Not applicable.</p>
      </sec>
      <sec>
        <title>AI and AI-assisted tools statement</title>
        <p>Not applicable.</p>
      </sec>
      <sec>
        <title>Financial support and sponsorship</title>
        <p>This work was supported by the National University of Singapore Start-up Grant (A-0010269-00-00).</p>
      </sec>
      <sec>
        <title>Conflicts of interest</title>
        <p>Both authors declared that there are no conflicts of interest.</p>
      </sec>
      <sec>
        <title>Ethical approval and consent to participate</title>
        <p>Not applicable.</p>
      </sec>
      <sec>
        <title>Consent for publication</title>
        <p>Not applicable.</p>
      </sec>
      <sec>
        <title>Copyright</title>
        <p>© The Author(s) 2026.</p>
      </sec>
    </sec>
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