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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Chem.</journal-id>
<journal-title>Frontiers in Chemistry</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Chem.</abbrev-journal-title>
<issn pub-type="epub">2296-2646</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">1023003</article-id>
<article-id pub-id-type="doi">10.3389/fchem.2022.1023003</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Chemistry</subject>
<subj-group>
<subject>Review</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Design, synthesis and application of two-dimensional metal tellurides as high-performance electrode materials</article-title>
<alt-title alt-title-type="left-running-head">Guo et al.</alt-title>
<alt-title alt-title-type="right-running-head">
<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.3389/fchem.2022.1023003">10.3389/fchem.2022.1023003</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Guo</surname>
<given-names>Meng</given-names>
</name>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Gu</surname>
<given-names>Shaonan</given-names>
</name>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1955152/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Xu</surname>
<given-names>Shuzheng</given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Lu</surname>
<given-names>Jiani</given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Wang</surname>
<given-names>Yinan</given-names>
</name>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Zhou</surname>
<given-names>Guowei</given-names>
</name>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1660818/overview"/>
</contrib>
</contrib-group>
<aff>
<institution>Key Laboratory of Fine Chemicals in Universities of Shandong</institution>, <institution>Jinan Engineering Laboratory for Multi-scale Functional Materials</institution>, <institution>School of Chemistry and Chemical Engineering</institution>, <institution>Qilu University of Technology (Shandong Academy of Sciences)</institution>, <addr-line>Jinan</addr-line>, <country>China</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1440079/overview">Hongda Li</ext-link>, Guangxi University of Science and Technology, China</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1885460/overview">Xintong Liu</ext-link>, Beijing Technology and Business University, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1872950/overview">Zhanglei Ning</ext-link>, Sichuan Normal University, China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Shaonan Gu, <email>sngu@qlu.edu.cn</email>; Guowei Zhou, <email>gwzhou@qlu.edu.cn</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Electrochemistry, a section of the journal Frontiers in Chemistry</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>26</day>
<month>09</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>10</volume>
<elocation-id>1023003</elocation-id>
<history>
<date date-type="received">
<day>19</day>
<month>08</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>31</day>
<month>08</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Guo, Gu, Xu, Lu, Wang and Zhou.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Guo, Gu, Xu, Lu, Wang and Zhou</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>Multifunctional electrode materials with inherent conductivity have attracted extensive attention in recent years. Two-dimensional (2D) metal telluride nanomaterials are more promising owing to their strong metallic properties and unique physical/chemical merits. In this review, recent advancements in the preparation of 2D metal tellurides and their application in electrode materials are presented. First, the most available preparation methods, such as hydro/solvent thermal, chemical vapor deposition, and electrodeposition, are summarized. Then, the unique performance of metal telluride electrodes in capacitors, anode materials of Li/Na ion batteries, electrocatalysis, and lithium-sulfur batteries are discussed. Finally, significant challenges and opportunities in the preparation and application of 2D metal tellurides are proposed.</p>
</abstract>
<kwd-group>
<kwd>2D metal tellurides</kwd>
<kwd>synthesis</kwd>
<kwd>electrocatalysis</kwd>
<kwd>batteries</kwd>
<kwd>electrodes</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>Increasing concerns about scarce resources and global climate issues have promoted the pursuit of clean and renewable energy for all humanity (<xref ref-type="bibr" rid="B13">Goodenough, 2014</xref>; <xref ref-type="bibr" rid="B76">Zeng et al., 2019</xref>). Many initiatives have attempted to power industrial civilization with renewable energy while ensuring the economic viability of related technologies, such as supercapacitors (SCs), alkali-ion batteries, lithium-sulfur (Li-S) batteries, etc., (<xref ref-type="bibr" rid="B24">Jaiswal, 2017</xref>; <xref ref-type="bibr" rid="B79">Zhang and Guo, 2020</xref>; <xref ref-type="bibr" rid="B10">Elmorshedy et al., 2021</xref>). Since then, electrode materials have emerged as a popular research topic in recent years. Many studies have attempted to improve the electrochemical characteristics of electrode materials by changing their composition, nano/microstructures, electronic properties, and so on (<xref ref-type="bibr" rid="B84">Zhang et al., 2019a</xref>; <xref ref-type="bibr" rid="B85">Zheng et al., 2021</xref>). However, as electrodes, one of the most important considerations is the inherent conductivity of the material.</p>
<p>Tellurium (Te), a sulfur element, has a higher conductivity compared with sulfur and selenium. It also has strong metallic characteristics, allowing telluride materials to admit more electrolyte ions and increase diffusion kinetics, enhancing energy storage reaction and offering high rate capability of energy storage devices (<xref ref-type="bibr" rid="B33">Kshetri et al., 2021</xref>). Owing to the unusual electrical structures and various two-dimensional (2D) crystals of 2D metal tellurides, these materials have recently received widespread attention as an essential component of metal chalcogenides (<xref ref-type="bibr" rid="B38">Li et al., 2016</xref>; <xref ref-type="bibr" rid="B2">Apte et al., 2018</xref>; <xref ref-type="bibr" rid="B32">Kononov et al., 2020</xref>; <xref ref-type="bibr" rid="B39">Liu et al., 2020</xref>). For instance, VTe<sub>2</sub> has excellent electrocatalytic activity for hydrogen evolution reactions and is regarded as a high-performance electrode material (<xref ref-type="bibr" rid="B55">Shi et al., 2021</xref>). In addition, NiTe, which has better conductivity and faster electron transfer capability compared with semiconductors, can maintain a specific capacity of approximately 307&#xa0;mAh g<sup>&#x2212;1</sup>&#xa0;at a high rate of 500&#xa0;mA&#xa0;g<sup>&#x2212;1</sup> as the anode of rechargeable aluminum ion batteries (<xref ref-type="bibr" rid="B75">Yu et al., 2020</xref>). Thus, the study of cathode materials for aluminum ion batteries and their use as battery anode materials [e.g., FeTe<sub>2</sub> (<xref ref-type="bibr" rid="B49">Park and Kang, 2020</xref>) and CoTe<sub>2</sub> (<xref ref-type="bibr" rid="B68">Yang et al., 2020</xref>)], electrocatalytic materials [e.g., Ni<sub>3</sub>Te<sub>2</sub> (<xref ref-type="bibr" rid="B6">De Silva et al., 2018</xref>) and MoTe<sub>2</sub> (<xref ref-type="bibr" rid="B90">Zhou et al., 2017a</xref>)], and SC materials [e.g., NiTe (<xref ref-type="bibr" rid="B4">Chen et al., 2019</xref>) and CoTe<sub>2</sub> (<xref ref-type="bibr" rid="B44">Manikandan et al., 2020</xref>)] is of great importance.</p>
<p>In recent years, tellurides have become widely used in electrochemistry owing to their 2D layered structure and unique properties (<xref ref-type="bibr" rid="B60">Wang et al., 2019</xref>; <xref ref-type="bibr" rid="B36">Li et al., 2020a</xref>; <xref ref-type="bibr" rid="B46">Myung et al., 2020</xref>; <xref ref-type="bibr" rid="B80">Zhang et al., 2021</xref>). On this basis, we provide a comprehensive overview of tellurides in this study, as shown in <xref ref-type="fig" rid="F1">Figure 1</xref>. We first focus on the preparation methods of telluride electrode materials, including chemical vapor deposition (CVD) (<xref ref-type="bibr" rid="B64">Wood et al., 2014</xref>; <xref ref-type="bibr" rid="B86">Zhou et al., 2017b</xref>; <xref ref-type="bibr" rid="B57">Tang et al., 2019</xref>; <xref ref-type="bibr" rid="B18">Hao et al., 2021</xref>; <xref ref-type="bibr" rid="B80">Zhang et al., 2021</xref>; <xref ref-type="bibr" rid="B91">Zhou et al., 2021</xref>), hydrothermal method (<xref ref-type="bibr" rid="B59">Wang et al., 2012</xref>; <xref ref-type="bibr" rid="B21">Hou et al., 2013</xref>; <xref ref-type="bibr" rid="B48">Oh et al., 2020</xref>; <xref ref-type="bibr" rid="B52">Qi et al., 2021</xref>), and electrodeposition (<xref ref-type="bibr" rid="B45">Morris and Vanderveen, 1993</xref>; <xref ref-type="bibr" rid="B74">Yu et al., 2018</xref>), and their electrochemical properties and applications. Subsequently, conceivable perspectives on the challenges and opportunities of 2D telluride electrode materials are proposed to provide insights into future research.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Overview framework of 2D metal telluride atomic crystals.</p>
</caption>
<graphic xlink:href="fchem-10-1023003-g001.tif"/>
</fig>
</sec>
<sec id="s2">
<title>2 Preparation</title>
<p>2D metal tellurides have recently become popular in energy devices such as SCs, photocatalysts, and electrode materials. Thus far, several preparation methods have been developed to synthesize 2D metal telluride nanomaterials, as summarized in <xref ref-type="table" rid="T1">Table 1</xref>.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Synthesis methods and application of metal tellurides.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Tellurides</th>
<th align="left">Applications</th>
<th align="left">Preparation method</th>
<th align="left">Morphology</th>
<th align="left">Temp (&#x25e6;C)</th>
<th align="left">Time (h)</th>
<th align="left">Ref</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td rowspan="2" align="left">Bi<sub>2</sub>Te<sub>3</sub>
</td>
<td align="left">-</td>
<td align="left">Hydrothermal</td>
<td align="left">Nanotubes</td>
<td align="left">180</td>
<td align="left">48</td>
<td align="left">
<xref ref-type="bibr" rid="B61">Wang et al. (2010)</xref>
</td>
</tr>
<tr>
<td align="left">Thermoelectric application</td>
<td align="left">Spark plasma sintering</td>
<td align="left">Nanosheet</td>
<td align="left">260</td>
<td align="left">-</td>
<td align="left">
<xref ref-type="bibr" rid="B31">Kim et al. (2021)</xref>
</td>
</tr>
<tr>
<td align="left">BiSbTe<sub>3</sub>
</td>
<td align="left">LIBs</td>
<td align="left">Solvothermal</td>
<td align="left">-</td>
<td align="left">180</td>
<td align="left">24</td>
<td align="left">
<xref ref-type="bibr" rid="B92">Zhu et al. (2020)</xref>
</td>
</tr>
<tr>
<td align="left">WTe<sub>2</sub>
</td>
<td align="left">Superconductors</td>
<td align="left">-</td>
<td align="left">Film</td>
<td align="left">350</td>
<td align="left">-</td>
<td align="left">
<xref ref-type="bibr" rid="B3">Asaba et al. (2018)</xref>
</td>
</tr>
<tr>
<td rowspan="3" align="left">CoTe<sub>2</sub>
</td>
<td align="left">-</td>
<td align="left">Solvothermal</td>
<td align="left">Nanotubes</td>
<td align="left">200</td>
<td align="left">24</td>
<td align="left">
<xref ref-type="bibr" rid="B35">Li et al. (2009)</xref>
</td>
</tr>
<tr>
<td align="left">Electrocatalyst</td>
<td align="left">Hydrothermal</td>
<td align="left">Nanoparticles</td>
<td align="left">180</td>
<td align="left">16</td>
<td align="left">
<xref ref-type="bibr" rid="B42">Lu et al. (2015)</xref>
</td>
</tr>
<tr>
<td align="left">Li-S batteries</td>
<td align="left">Hydrothermal</td>
<td align="left">-</td>
<td align="left">200</td>
<td align="left">24</td>
<td align="left">
<xref ref-type="bibr" rid="B56">Song et al. (2021)</xref>
</td>
</tr>
<tr>
<td align="left">MoTe<sub>2</sub>
</td>
<td align="left">Li-S batteries</td>
<td align="left">Hydrothermal</td>
<td align="left">-</td>
<td align="left">200</td>
<td align="left">36</td>
<td align="left">
<xref ref-type="bibr" rid="B73">Yu et al. (2021)</xref>
</td>
</tr>
<tr>
<td align="left"/>
<td align="left">Photocatalysts</td>
<td align="left">Hydrothermal</td>
<td align="left">-</td>
<td align="left">200</td>
<td align="left">48</td>
<td align="left">
<xref ref-type="bibr" rid="B34">Li et al. (2020b)</xref>
</td>
</tr>
<tr>
<td align="left">VTe<sub>2</sub>
</td>
<td align="left">Li-S batteries</td>
<td align="left">CVD</td>
<td align="left">-</td>
<td align="left">&#x223c;650</td>
<td align="left">-</td>
<td align="left">
<xref ref-type="bibr" rid="B60">Wang et al. (2019)</xref>
</td>
</tr>
<tr>
<td rowspan="3" align="left">Sb<sub>2</sub>Te<sub>3</sub>
</td>
<td align="left">LIBs</td>
<td align="left">Mixing</td>
<td align="left">-</td>
<td align="left">-</td>
<td align="left">-</td>
<td align="left">
<xref ref-type="bibr" rid="B14">Grishanov et al. (2018a)</xref>
</td>
</tr>
<tr>
<td align="left">-</td>
<td align="left">Microwave-assisted Solvothermal</td>
<td align="left">Various morphologies</td>
<td align="left">-</td>
<td align="left">-</td>
<td align="left">
<xref ref-type="bibr" rid="B8">Dong et al. (2011)</xref>
</td>
</tr>
<tr>
<td align="left">LIBs</td>
<td align="left">Ball milling</td>
<td align="left">Micro-particles</td>
<td align="left">-</td>
<td align="left">12</td>
<td align="left">
<xref ref-type="bibr" rid="B62">Wei et al. (2020)</xref>
</td>
</tr>
<tr>
<td align="left">Ge<sub>2</sub>Sb<sub>2</sub>T<sub>5</sub>
</td>
<td align="left">LIBs</td>
<td align="left">Ball milling</td>
<td align="left">-</td>
<td align="left">-</td>
<td align="left">40</td>
<td align="left">
<xref ref-type="bibr" rid="B63">Wei et al. (2019)</xref>
</td>
</tr>
<tr>
<td rowspan="2" align="left">NiTe</td>
<td align="left">Supercapacitor Electrode material</td>
<td align="left">Solvothermal</td>
<td align="left">Nanoplates</td>
<td align="left">200</td>
<td align="left">20</td>
<td align="left">
<xref ref-type="bibr" rid="B4">Chen et al. (2019)</xref>
</td>
</tr>
<tr>
<td align="left"/>
<td align="left">Hydrothermal</td>
<td align="left">Network</td>
<td align="left">180</td>
<td align="left">18</td>
<td align="left">
<xref ref-type="bibr" rid="B7">Deshagani et al. (2020)</xref>
</td>
</tr>
<tr>
<td align="left">SnTe</td>
<td align="left">LIBs</td>
<td align="left">Hydrogen peroxide</td>
<td align="left">-</td>
<td align="left">-</td>
<td align="left">-</td>
<td align="left">
<xref ref-type="bibr" rid="B15">Grishanov et al. (2018b)</xref>
</td>
</tr>
<tr>
<td align="left">Cu<sub>2</sub>Te</td>
<td align="left">-</td>
<td align="left">Electrodeposition</td>
<td align="left">-</td>
<td align="left">-</td>
<td align="left">-</td>
<td align="left">
<xref ref-type="bibr" rid="B23">Ishizaki et al. (2003)</xref>
</td>
</tr>
<tr>
<td align="left">Cu<sub>(2-x)</sub>Te</td>
<td align="left">Chemotherapy</td>
<td align="left">Bio-synthesis</td>
<td align="left">Nanocubes</td>
<td align="left">160</td>
<td align="left">0.75</td>
<td align="left">
<xref ref-type="bibr" rid="B51">Poulose et al. (2016)</xref>
</td>
</tr>
<tr>
<td align="left">ZnTe</td>
<td align="left">Bio-imaging and bio-labeling</td>
<td align="left">Bio-synthesis</td>
<td align="left">Nanoparticles</td>
<td align="left">-</td>
<td align="left">-</td>
<td align="left">
<xref ref-type="bibr" rid="B9">Dunpall et al. (2014)</xref>
</td>
</tr>
<tr>
<td align="left">MnTe</td>
<td align="left">Optoelectronic devices</td>
<td align="left">CVD</td>
<td align="left">Nanosheet</td>
<td align="left">580</td>
<td align="left">-</td>
<td align="left">
<xref ref-type="bibr" rid="B36">Li et al. (2020a)</xref>
</td>
</tr>
<tr>
<td align="left">In<sub>2</sub>Te<sub>3</sub>
</td>
<td align="left">Gas sensing and hydrogen storage</td>
<td align="left">Solvothermal</td>
<td align="left">Nanotubes</td>
<td align="left">180</td>
<td align="left">48</td>
<td align="left">
<xref ref-type="bibr" rid="B88">Zhou et al. (2014)</xref>
</td>
</tr>
</tbody>
</table>
</table-wrap>
<sec id="s2-1">
<title>2.1 Hydro/solvothermal methods</title>
<p>The most prevalent techniques for synthesizing nanomaterials are the hydrothermal and solvothermal procedures. In contrast to alternative procedures for synthesizing nanostructured materials, the hydrothermal approach offers the benefits of low synthesis temperature and small grain size. This approach may produce a wide range of morphologies, including nanorods (<xref ref-type="bibr" rid="B75">Yu et al., 2020</xref>; <xref ref-type="bibr" rid="B27">Jayababu et al., 2021</xref>), nanosheets (<xref ref-type="bibr" rid="B42">Lu et al., 2015</xref>; <xref ref-type="bibr" rid="B34">Li et al., 2020b</xref>), nanowires (<xref ref-type="bibr" rid="B69">Yang et al., 2009</xref>; <xref ref-type="bibr" rid="B58">Wan et al., 2011</xref>), and nanotubes (<xref ref-type="bibr" rid="B61">Wang et al., 2010</xref>). Moreover, in contrast to other synthesis methods, the hydrothermal approach has an excessively high oxygen affinity for positively charged metal and negatively charged Te ions, resulting in the formation of oxides. Reducing agents, such as hydrazine and sodium borohydride, are necessary to avoid oxide impurities in tellurides.</p>
<p>Wang et al. adopted the hydrothermal technique to synthesize Bi<sub>2</sub>Te<sub>3</sub> nanotubes with diameters of 100&#xa0;nm and lengths of 500&#x2013;1,000&#xa0;nm by using sodium borohydride as the reducing agent and EDTA as the surfactant (<xref ref-type="fig" rid="F2">Figure 2A&#x2013;D</xref>) (<xref ref-type="bibr" rid="B61">Wang et al., 2010</xref>). Zhang et al. created carbon-encapsulated porous Sb<sub>2</sub>Te<sub>3</sub> nanoplates with porous architectures <italic>via</italic> the hydrothermal and carbonization processes, with carbon shell thicknesses ranging from 50 to 80&#xa0;nm (<xref ref-type="fig" rid="F2">Figures 2E&#x2013;J</xref>) (<xref ref-type="bibr" rid="B82">Zhang et al., 2019b</xref>). Their approach can successfully produce nanomaterials, such as Ag<sub>2</sub>Te (<xref ref-type="bibr" rid="B78">Zhang et al., 2006</xref>), Bi<sub>2</sub>Te<sub>3</sub> (<xref ref-type="bibr" rid="B61">Wang et al., 2010</xref>), CdTe (<xref ref-type="bibr" rid="B12">Gong et al., 2011</xref>), Cu<sub>2</sub>Te (<xref ref-type="bibr" rid="B78">Zhang et al., 2006</xref>), Cu<sub>2-x</sub>Te (<xref ref-type="bibr" rid="B25">Jamwal et al., 2016a</xref>), HgTe (<xref ref-type="bibr" rid="B54">Salavati-Niasari et al., 2010</xref>), NiTe (<xref ref-type="bibr" rid="B77">Zhang et al., 2002</xref>), and PbTe (<xref ref-type="bibr" rid="B26">Jamwal et al., 2016b</xref>).</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>
<bold>(A&#x2013;D)</bold> TEM, SAED pattern, and SEM images of the Bi<sub>2</sub>Te<sub>3</sub> (<xref ref-type="bibr" rid="B61">Wang et al., 2010</xref>). Copyright 2010, Elsevier. <bold>(E&#x2013;J)</bold> morphologies and Te, Sb, C elemental mapping of the as-prepared Sb<sub>2</sub>Te<sub>3</sub>@C sample (<xref ref-type="bibr" rid="B82">Zhang et al., 2019b</xref>). Copyright 2019, American Chemical Society. <bold>(K)</bold> SEM of BiSbTe<sub>3</sub> nanosheets. <bold>(L)</bold> TEM and <bold>(M)</bold> HRTEM images of BiSbTe<sub>3</sub>/N-rGO (<xref ref-type="bibr" rid="B92">Zhu et al., 2020</xref>). Copyright 2020, Elsevier.</p>
</caption>
<graphic xlink:href="fchem-10-1023003-g002.tif"/>
</fig>
<p>Similar advantages can be attained in solvothermal reactions, such as when one or more precursors are dissolved in a non-aqueous solvent. The BiSbTe<sub>3</sub> nanosheets were prepared under solvent-heated conditions by using ethylene glycol as the solvent (<xref ref-type="fig" rid="F2">Figures 2K&#x2013;M</xref>) (<xref ref-type="bibr" rid="B92">Zhu et al., 2020</xref>). The unique nano-plate structure of BiSbTe<sub>3</sub> increases the exposure of the electrolyte, leading to high utilization of the composite electrode material during cycling. In addition, the solvothermal method is also commonly used to prepare other metal tellurides, such as Bi<sub>2</sub>Te<sub>3</sub> (<xref ref-type="bibr" rid="B41">Liu et al., 2017a</xref>), Cu<sub>
<italic>x</italic>
</sub>Te (<xref ref-type="bibr" rid="B41">Liu et al., 2017a</xref>), PbTe (<xref ref-type="bibr" rid="B41">Liu et al., 2017a</xref>), Ag<sub>2</sub>Te (<xref ref-type="bibr" rid="B41">Liu et al., 2017a</xref>), and Sb<sub>2</sub>Te<sub>3</sub> (<xref ref-type="bibr" rid="B67">Yan et al., 2016</xref>).</p>
</sec>
<sec id="s2-2">
<title>2.2 Chemical vapor deposition methods</title>
<p>CVD is generally used to create thin film materials. This approach is based on the principle of utilizing gaseous precursor reactants to produce thin films on a substrate by breaking down specific components of the gaseous precursor <italic>via</italic> atomic and intermolecular chemical interactions (<xref ref-type="bibr" rid="B87">Zhou et al., 2015</xref>; <xref ref-type="bibr" rid="B47">Naylor et al., 2016</xref>; <xref ref-type="bibr" rid="B86">Zhou et al., 2017b</xref>; <xref ref-type="bibr" rid="B72">Yoo et al., 2017</xref>). The form and properties of the 2D metal tellurides are influenced by the substrates, precursors, and temperature, among other factors (<xref ref-type="bibr" rid="B89">Zhou et al., 2016</xref>; <xref ref-type="bibr" rid="B83">Zhang et al., 2019c</xref>; <xref ref-type="bibr" rid="B22">Huang et al., 2019</xref>; <xref ref-type="bibr" rid="B30">Kim et al., 2020</xref>). CVD method is the most widely used method for the synthesis of tellurides, which has good scalability and can be controlled to prepare large-area films or two-dimensional crystals.</p>
<p>Recently, MoTe<sub>2</sub> has received widespread attention owing to its distinct semiconducting and semi-metallic characteristics. Kong et al. investigated a CVD technique for fabricating uniform high-crystalline 2H and 1T&#x27;-MoTe<sub>2</sub> films (<xref ref-type="bibr" rid="B47">Naylor et al., 2016</xref>). Various products were created by varying the precursor, carrier gas, and temperature. Under the same conditions, they observed that MoO<sub>3</sub> precursors converted more easily into 2H-MoTe<sub>2</sub>, whereas MoO and MoO<sub>x</sub> (x &#x3c; 3) precursors converted more effectively into 1T&#x27;-MoTe<sub>2</sub>. A year later, Kong et al. improved the preparation process and successfully synthesized large-size homogeneous 1T&#x27;-MoTe<sub>2</sub> (<xref ref-type="bibr" rid="B89">Zhou et al., 2016</xref>). They further determined the significant effect of the molybdenum precursor on the formation of 1T&#x27;-MoTe<sub>2</sub> (<xref ref-type="fig" rid="F3">Figure 3A&#x2013;E</xref>). 1T&#x27;-MoTe<sub>2</sub> was reliably created when MoO<sub>3</sub> was utilized as a precursor. Furthermore, the amount of Te used in the synthesis of 1T&#x27;-MoTe<sub>2</sub> had a substantial impact. If the Te supply is sufficient, then 2H-MoTe<sub>2</sub> would be produced; otherwise 1T&#x27;-MoTe<sub>2</sub> would be produced (<xref ref-type="bibr" rid="B89">Zhou et al., 2016</xref>). The established CVD technique also allowed for the large-scale direct synthesis of WTe<sub>2</sub> and MoTe<sub>2</sub> multilayers and monolayers (<xref ref-type="bibr" rid="B86">Zhou et al., 2017b</xref>). The thickness of the WTe<sub>2</sub> and MoTe<sub>2</sub> atomic layers was adjusted using growth time. (<xref ref-type="fig" rid="F3">Figure 3F&#x2013;M</xref>).</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>
<bold>(A)</bold> Schematic illustration of CVD method to deposit 1T&#x2032; and 2H MoTe<sub>2</sub> films. <bold>(B)</bold> high-resolution TEM image, and <bold>(C)</bold> SAED pattern of 1T&#x2032;- MoTe<sub>2</sub> film grown from MoO<sub>3</sub>; <bold>(D)</bold> Typical optical and <bold>(E)</bold> AFM image of a 1T&#x2032;- MoTe<sub>2</sub> film (<xref ref-type="bibr" rid="B89">Zhou et al., 2016</xref>). Copyright 2016, Wiley-VCH. <bold>(F)</bold> Schematic illustration of CVD method to grow WTe<sub>2</sub> and MoTe<sub>2</sub> atomic layers. <bold>(G,H)</bold> Crystalline structures of 1T&#x2032;-W(Mo)Te<sub>2</sub>. <bold>(I,J)</bold> Optical images of MoTe<sub>2</sub> and WTe<sub>2</sub> monolayer. <bold>(K)</bold> Optical image of a MoTe<sub>2</sub> flake containing 1, 2, and 3&#xa0;L MoTe<sub>2</sub>. <bold>(L,M)</bold> Optical images of a large scale monolayer and bilayer WTe<sub>2</sub> films (<xref ref-type="bibr" rid="B86">Zhou et al., 2017b</xref>). Copyright 2017, Wiley-VCH.</p>
</caption>
<graphic xlink:href="fchem-10-1023003-g003.tif"/>
</fig>
<p>In addition to 2D WTe<sub>2</sub> and MoTe<sub>2</sub>, many other 2D transition metal tellurides can be grown <italic>via</italic> CVD methods. Li et al. reported a method that can precisely control 2H-MoTe defects grown by a large-scale phase-change-assisted CVD process using selective etching of I<sub>3</sub>
<sup>&#x2212;</sup> solutions (<xref ref-type="bibr" rid="B91">Zhou et al., 2021</xref>). Liu et al. reported a facile CVD method to synthesize Mo<sub>x</sub>W<sub>1-x</sub>Te<sub>2</sub> with controlled thickness and chemical composition ratios to investigate its design of material devices from a topological quantum state perspective (<xref ref-type="bibr" rid="B5">Chubilleau et al., 2011</xref>). Li et al. reported a strategy using mixed molten salts for enhancing the CVD growth of 2D WTe<sub>2</sub> crystals with large grain size and yield, acting as a synergist (<xref ref-type="bibr" rid="B27">Jayababu et al., 2021</xref>).</p>
</sec>
<sec id="s2-3">
<title>2.3 Electrochemical deposition method</title>
<p>Electrochemical deposition (ECD) is another effective method for obtaining metal tellurides. ECD has the outstanding advantage of easily controlling the morphologies of metal tellurides by using removable templates. Compared with other methods, the ECD method is simple, not limited by grain size and shape, and the prepared crystalline materials have unique properties. Applied electrical potential and deposition rate are two critical parameters of smooth ECD.</p>
<p>Islam et al. suggested an ECD technique for handling bespoke Al<sub>2</sub>O<sub>3</sub> (AAO) stencils that neither needed extensive hole branching nor would damage the aluminum substrate(<xref ref-type="fig" rid="F4">Figure 4</xref>) (<xref ref-type="bibr" rid="B65">Wu et al., 2020</xref>). CdTe nanotubes have a high aspect ratio of one-dimensional nanostructures compared to other nanostructures and have amplified optical waveguide properties. Therefore, they are designed as visible light responsive photocatalysts. <xref ref-type="fig" rid="F4">Figure 4A</xref> shows that CdTe was electrochemically deposited onto tailored AAO stencils, which has been sheared by utilizing the full AAO to allow for the acquisition of through-hole and self-supporting features on the Al substrate. The CdTe nanotubes developed in the sulfate bath after the barrier layer has been completely removed, as shown in <xref ref-type="fig" rid="F4">Figure 4B</xref>. The image within the red border is a magnified view of the designated section in the red circle, revealing the hollow ends of the vertically aligned nanotubes. This feature implies the significant advantage of the material to provide electrical contact during cathodic deposition because the aluminum base remains intact even after the barrier layer is completely removed. Meanwhile, broaching barrier layer (BBL) was polarized in dilute H<sub>2</sub>SO<sub>4</sub>, compared to neutral KCl solution and immersion in H<sub>3</sub>PO<sub>4</sub> solution, resulting in a totally etched barrier layer that was innocuous to the substrate aluminum.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>
<bold>(A)</bold> Schematic illustration of the steps involved to remove barrier layer from AAO template keeping base Al intact for electrodeposition of CdTe nanotubes; and <bold>(B)</bold> FE-SEM micrograph of CdTe nanotubes deposited in BL removed AAO template. <bold>(C)</bold> TEM images illustrating CdTe hollow nanotubes; and <bold>(D)</bold> solid nanorod obtained using sulfate electrolyte bath (<xref ref-type="bibr" rid="B65">Wu et al., 2020</xref>). Copyright 2019, Elsevier.</p>
</caption>
<graphic xlink:href="fchem-10-1023003-g004.tif"/>
</fig>
<p>Choa et al. converted Ag<sub>2</sub>Te nanotubes to PbTe nanotubes by changing the silver-to-lead atomic ratio through the combined processes of electrostatic spinning, ECD, and cation exchange (<xref ref-type="fig" rid="F5">Figures 5A&#x2013;F</xref>) (<xref ref-type="bibr" rid="B7">Deshagani et al., 2020</xref>). Silver atoms were diffused into the Te layer and transformed into Ag<sub>2</sub>Te nanofibers by ECD using silver nanofibers synthesized by electrostatic spinning as the starting material. Then, the crystalline transition of Ag<sub>x</sub>Te<sub>y</sub> to PbTe nanocomposites was controlled by the cation exchange from Ag<sup>&#x2b;</sup> cations to Pb<sup>2&#x2b;</sup> cations.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>SEM images of <bold>(A)</bold> Ag nanofibers; <bold>(B)</bold> Ag<sub>2</sub>Te nanotubes and <bold>(C)</bold> PbTe nanotubes; <bold>(D&#x2013;F)</bold> EDS mapping (<xref ref-type="bibr" rid="B7">Deshagani et al., 2020</xref>). Copyright 2018, Elsevier. <bold>(G)</bold> Schematic illustration of the synthetic process of CoTe<sub>2</sub>-C composite (<xref ref-type="bibr" rid="B68">Yang et al., 2020</xref>). Copyright 2020, Elsevier.</p>
</caption>
<graphic xlink:href="fchem-10-1023003-g005.tif"/>
</fig>
<p>In addition to the abovementioned three methods, many other chemical routes can be used to extensively investigate the synthesis of metal telluride nanomaterials. Examples are microwave synthesis (<xref ref-type="bibr" rid="B71">Ye et al., 2019</xref>), spray pyrolysis (<xref ref-type="bibr" rid="B4">Chen et al., 2019</xref>), biosynthesis (<xref ref-type="bibr" rid="B51">Poulose et al., 2016</xref>), and laser ablation techniques (<xref ref-type="bibr" rid="B28">Jayababu and Kim, 2021</xref>). A good method allows for the accurate control of certain features, including spatial structure and distribution, which significantly impact the performance of electrode materials. Kang et al. investigated anode materials for potassium ion batteries using spray pyrolysis to make cobalt telluride-C (CoTe<sub>2</sub>-C) composite microspheres, as shown in <xref ref-type="fig" rid="F5">Figure 5G</xref>, (<xref ref-type="bibr" rid="B68">Yang et al., 2020</xref>). As Te needed to be directly embedded into the composite microspheres, a simple one-step post-treatment technique was used to prepare CoTe<sub>2</sub>-C composite microspheres. Their approach could be explained by Ostwald maturation induced by the formation of the CoTe<sub>2</sub> crystals.</p>
</sec>
</sec>
<sec id="s3">
<title>3 Applications as electrodes</title>
<sec id="s3-1">
<title>3.1 Supercapacitor</title>
<p>Telluride has a substantially greater electrical conductivity and is projected to perform better electrochemically compared with other materials, leading to the widespread research and advancement of metal tellurides built into diverse nanostructures for supercapacitor (SC) applications (<xref ref-type="bibr" rid="B40">Liu et al., 2017b</xref>; <xref ref-type="bibr" rid="B53">Rathore et al., 2022</xref>). Kim et al. created silver-decorated NiFe alloy telluride nanorods (AMMT HNRs) on nickel foam (NF) (<xref ref-type="fig" rid="F6">Figure 6A</xref>) (<xref ref-type="bibr" rid="B27">Jayababu et al., 2021</xref>). The robust electroactivity of the NiFe alloy, the high conductivity of Te and Ag, and the porous layered structure of the telluride all contributed to the AMMT HNRs/NF electrode&#x2019;s outstanding electrochemical performance. The electrode exhibited a stability of 80.4% over 3,000 cycles. After employing AMMT HNRs/NF and carbon-coated NF as positive and negative electrodes, respectively, and cellulose membranes as separators, high areal energy and power densities were reported in hybrid supercapacitors. (<xref ref-type="fig" rid="F6">Figure 6B</xref>).</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>
<bold>(A)</bold> Schematic of the MMT HNRs/NF and AMMT HNRs/NF electrodes; <bold>(B)</bold> Schematic of the hybrid supercapacitors; <bold>(C)</bold> Energy and power density of the hybrid supercapacitors and real-time suitability tests as a digital multi-sensor power supply (<xref ref-type="bibr" rid="B27">Jayababu et al., 2021</xref>). Copyright 2021, American Chemical Society. <bold>(D)</bold> Step by step illustration of NT and NST electrodes&#x2019; electrochemical processes. <bold>(E)</bold> Electrochemical performance of NiS/NiTe/Ni//AC asymmetric supercapacitor electrodes up to over 200 000 cycles at different current densities (<xref ref-type="bibr" rid="B4">Chen et al., 2019</xref>). Copyright 2019, Elsevier.</p>
</caption>
<graphic xlink:href="fchem-10-1023003-g006.tif"/>
</fig>
<p>NiTe, as an SC electrode material, has also attracted the interest of scientists (<xref ref-type="bibr" rid="B50">Park et al., 2018</xref>; <xref ref-type="bibr" rid="B56">Song et al., 2021</xref>; <xref ref-type="bibr" rid="B73">Yu et al., 2021</xref>). The NiTe achieved outstanding electrochemical performance as a coexisting pseudo capacitive material for NiS reported by Wu et al. (<xref ref-type="bibr" rid="B4">Chen et al., 2019</xref>). As shown in <xref ref-type="fig" rid="F6">Figure 6D</xref>, four electrochemical reactions occurred on the NiS/NiTe/Ni (NST) electrode. During charging, the volume increased from the inner layer to the outer layer; during discharge, the volume was reduced from the outer layer to the inner layer. The NST was the positive electrode of the asymmetric SC, whereas the active carbon (AC) was the negative electrode. The high capacitance retention and ultra-long cycle life (200000 cycles, <xref ref-type="fig" rid="F6">Figure 6E</xref>) demonstrated the important role of the synergistic structure to structural stability. Additionally, CoTe<sub>2</sub> (<xref ref-type="bibr" rid="B44">Manikandan et al., 2020</xref>), CuCoTe (<xref ref-type="bibr" rid="B11">Fu and Lee, 2019</xref>), VTe<sub>2</sub> (<xref ref-type="bibr" rid="B1">Ahmad et al., 2021</xref>), and MoTe<sub>2</sub> (<xref ref-type="bibr" rid="B29">Jin et al., 2018</xref>) have been widely used as electrode materials for high-performance capacitors.</p>
</sec>
<sec id="s3-2">
<title>3.2 Anode materials</title>
<p>Metal tellurides have emerged as the most feasible alternative for cutting-edge ion battery anode materials because to their layered crystal structure, high intrinsic conductivity, and high trap density (<xref ref-type="bibr" rid="B92">Zhu et al., 2020</xref>; <xref ref-type="bibr" rid="B16">Guo et al., 2021</xref>; <xref ref-type="bibr" rid="B19">Hassan et al., 2021</xref>). Kang et al. used a structurally distinct FeTe<sub>2</sub> and carbon nanocomposite as anode material for potassium ion batteries (<xref ref-type="fig" rid="F7">Figure 7</xref>) (<xref ref-type="bibr" rid="B49">Park and Kang, 2020</xref>). The hollow carbon nanospheres that housed the iron telluride nanocrystals (FeTe<sub>2</sub>-C) offered enough space to accommodate for the nanocrystals&#x2019; enormous volume variations during charging and discharging. During cycling, nanocrystal extrusion within the solid hollow carbon nanospheres was controlled, and no FeTe<sub>2</sub> from the electrode were lost, showing strong structural integrity (<xref ref-type="bibr" rid="B49">Park and Kang, 2020</xref>). Kang et al. also investigated the reaction mechanism of the CoTe<sub>2</sub>-C composite microsphere as an anode material for potassium ion batteries and the related potassium ion conversion. Where the mechanism of the CoTe<sub>2</sub> phase transition reaction can be expressed as:<disp-formula id="equ1">
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<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>
<bold>(A)</bold> Formation illustration of the hollow carbon nanosphere within FeTe<sub>2</sub>-C nanospheres: <bold>(B&#x2013;D)</bold> SEM and TEM images of initial FeTe<sub>2</sub>-C and FeTe<sub>2</sub>-C after cycled. <bold>(E)</bold> long-term cycling performances of FeTe<sub>2</sub> and FeTe<sub>2</sub>-C (<xref ref-type="bibr" rid="B49">Park and Kang, 2020</xref>). Copyright 2020, Wiley-VCH.</p>
</caption>
<graphic xlink:href="fchem-10-1023003-g007.tif"/>
</fig>
<p>The surface-driven reactions during rapid potassiumization/depotassiumization significantly promote the charge storage of CoTe<sub>2</sub>-C in potassium ion cells, leading to excellent rate performance. And the high contribution of the capacitance-controlled behavior of CoTe<sub>2</sub>-C indicates its good multiplicative performance. At a current density of 0.5&#xa0;A&#xa0;g<sup>&#x2212;1</sup>, the CoTe<sub>2</sub>-C composite has a 100th cycle discharge capacity of 189.5&#xa0;mAh g<sup>&#x2212;1</sup> (<xref ref-type="bibr" rid="B4">Chen et al., 2019</xref>). In addition, Kim et al. (<xref ref-type="bibr" rid="B11">Fu and Lee, 2019</xref>) investigated a CuCo LDHs-coated CuCoTe honeycomb nanosheet as anode for hybrid SCs. They demonstrated the material&#x2019;s excellent electrochemical performance and high stability (<xref ref-type="bibr" rid="B4">Chen et al., 2019</xref>).</p>
</sec>
<sec id="s3-3">
<title>3.3 Electrocatalysis</title>
<p>Depicted as 2D materials, tellurides have also been recently described as electrocatalytically active materials with low cost and strong catalytic activity (<xref ref-type="bibr" rid="B43">Luxa et al., 2017</xref>; <xref ref-type="bibr" rid="B17">Han et al., 2020</xref>). Nath et al. used hydrothermal and electrodeposition methods to create 5 and 8&#xa0;nm-thick Ni<sub>3</sub>Te<sub>2</sub> films (<xref ref-type="bibr" rid="B6">De Silva et al., 2018</xref>). Voltammetric cycling and linear sweep voltammetry were used to examine the OER catalytic activity of the as-synthesized materials in the alkaline electrolytes. Their results showed that Ni<sub>3</sub>Te<sub>2</sub> films have a high catalytic efficiency of 10&#xa0;mA&#xa0;cm<sup>&#x2212;2</sup> with a notably low overpotential of 180&#xa0;mV. The overpotential value was much lower than that needed for nanostructured Ni<sub>3</sub>Se<sub>2</sub> (190&#xa0;mV) (<xref ref-type="bibr" rid="B66">Xu et al., 2019</xref>) and Ni<sub>3</sub>S<sub>2</sub> (260&#xa0;mV) (<xref ref-type="bibr" rid="B37">Li et al., 2022</xref>). Nanodendritic MoTe<sub>2</sub> was used as an electrocatalyst for hydrogen precipitation reaction (<xref ref-type="bibr" rid="B90">Zhou et al., 2017a</xref>). Nanodendrimers were created electrochemically on Mo-doped reduced polyimide/graphene oxide composite substrates. The deposition period increased the size of the nanodendrites. Their findings further showed that nanodendrimers have the potential to be good catalysts for hydrogen precipitation in neutral fluids. Ashiq et al. proposed a highly active Cu<sub>7</sub>Te<sub>4</sub> nanowire synthesized through water oxidation as an electrocatalyst for water oxidation reaction (<xref ref-type="bibr" rid="B81">Zhang et al., 2022</xref>). Chu et al. demonstrated the ability of FeTe<sub>2</sub> to function as an efficient and durable nitrogen reduction electrocatalyst, with an excellent combination of NH<sub>3</sub> yield and Faraday efficiency (<xref ref-type="bibr" rid="B70">Yao et al., 2022</xref>). Metal telluride materials, such as Sb<sub>2</sub>Te<sub>3</sub> (<xref ref-type="bibr" rid="B20">He et al., 2022</xref>), MoTe<sub>2</sub>[99], Ni<sub>3</sub>Te<sub>2</sub>-CoTe[100], and NiTe-HfTe<sub>2</sub>[101], have received extensive attention for their potential application in electrocatalysis.</p>
</sec>
<sec id="s3-4">
<title>3.4 Li-S batteries</title>
<p>Because of its low cost, environmental friendliness, and high energy density, Li-S batteries are appealing next-generation energy storage technologies. Meanwhile, owing to the intrinsic 2D structure of telluride, it offers an interesting function in Li-S batteries (<xref ref-type="bibr" rid="B60">Wang et al., 2019</xref>; <xref ref-type="bibr" rid="B16">Guo et al., 2021</xref>; <xref ref-type="bibr" rid="B19">Hassan et al., 2021</xref>).</p>
<p>Xie et al. examined diphenyl ditelluride (DPDTe) as bifunctional electrolyte additive for high-efficiency sulfur cathodes and dendrite-free lithium anodes[102]. As shown in <xref ref-type="fig" rid="F8">Figures 8A&#x2013;E</xref>, the presence of DPDTe enables catalytic mediation by Te radicals, which is accountable for substantially enhancing LIPS redox dynamics and regulating Li<sub>2</sub>S accumulation. DPDTe can also combine with metallic lithium to generate a uniform, dense, and stable organic&#x2013;inorganic hybrid SEI to minimize the nucleation overpotential of lithium and promote uniform lithium deposition, thereby successfully limiting the formation of lithium dendrites. The addition of DPDTe can improve sulfur usage and lead to highly reversible lithium stripping/plating, further resulting in good rate capability (611.4&#xa0;mAh g<sup>&#x2212;1</sup>&#xa0;at 5C) of Li-S batteries.</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>
<bold>(A&#x2013;C)</bold> Electrochemical performance of Li&#x2013;S pouch cells with/without DPDTe additive, with high sulfur loading of 5&#xa0;mg&#xa0;cm<sup>&#x2212;2</sup> and E/S ratio of 5.0&#xa0;&#x3bc;L&#xa0;mg<sup>&#x2212;1</sup>. <bold>(D)</bold> SEM images of the Li<sub>2</sub>S deposition with DPDTe and <bold>(E)</bold> the cycled Li anode with DPDTe additive at the 50th cycle[102]. Copyright 2022, Wiley-VCH. <bold>(F,G)</bold> <italic>In situ</italic> Raman contour plots and Raman spectra at 0.1&#xa0;C with MSC/P&#x2282;NiTe<sub>2&#x2212;x</sub>; <bold>(H,I)</bold> Galvanostatic discharge/charge profiles and corresponding <italic>ex situ</italic> XANES of the S K-edge cathode with MSC/P&#x2282;NiTe<sub>2&#x2212;x</sub> separator; <bold>(J)</bold> Adsorption-catalytic LiPS mechanism with MSC/P&#x2282;NiTe<sub>2&#x2212;x</sub> in a Li&#x2013;S configuration[103]. Copyright 2022, Wiley-VCH.</p>
</caption>
<graphic xlink:href="fchem-10-1023003-g008.tif"/>
</fig>
<p>Zhan et al. explored a phosphorus-doped nickel Te electrocatalyst (P&#x2282;NiTe<sub>2-x</sub>) grown on carbon-based (MSC) as a functional layer for high-performance Li-S battery separators (MSC/P&#x2282;NiTe<sub>2-x</sub>)[103]. The increased electrochemical performance implies that the P doping of Te vacancies can enhance Li-S battery conductivity, boost adsorption, and decrease the redox energy barrier of Li-S batteries. MSC nanosheets enable NiTe<sub>2</sub> nanoparticles to disperse and diffuse Li<sup>&#x2b;</sup>. <italic>Ex-situ</italic> X-ray absorption spectroscopy and <italic>in-situ</italic> Raman spectroscopy both demonstrated the ability of MSC/P&#x2282;NiTe<sub>2-x</sub> to inhibit the shuttle effect and accelerate the redox conversion (<xref ref-type="fig" rid="F8">Figures 8F&#x2013;J</xref>). Compounding telluride materials in the electrode[91, 104], electrolyte, and diaphragm coatings has become one of the important strategies of breaking through the severe shuttle effect of Li-S batteries.</p>
</sec>
</sec>
<sec id="s4">
<title>4 Summary and prospective</title>
<p>Metal tellurides have received extensive attention owing to their great application potential for high-performance electrode materials. In this study, the synthesis methods of tellurides and the research progress of their properties and application in the field of electrodes were reviewed. Three methods for preparing metal tellurides were discussed. Then, the latest progress in terms of the role of telluride in capacitors, anode materials, electrocatalysis, and Li-S batteries was presented. Despite significant progress in the study of 2D tellurides, researchers still face considerable opportunities and challenges.</p>
<p>The CVD approach is now being widely utilized to controllably prepare tellurides. It is feasible to produce 2D tellurides with customizable shape and good crystallinity on a large scale. However, for powder electrochemical materials, the mild chemical interaction between the transition metal and Te under vapor conditions, on the other hand, is a disadvantage of CVD synthesis. Furthermore, while tellurides exhibit remarkable performance, they are difficult to precisely control properties such as pore structure and distribution in the preparation of electrode materials, which greatly affects the volume change of electrode materials during cycling, making it more difficult to improve the capacity, stability and extended cycle life of capacitors and batteries. Future studies should concentrate on: 1) investigating more approaches for the controlled synthesis of tellurides, not only for 2D single-crystal; and 2) designing more composites or building heterostructures to facilitate the electrochemical performances telluride-based electrodes, because like other sulfide generics, tellurides also suffer from extreme volume fluctuations, which result in poor cycling performance.</p>
</sec>
</body>
<back>
<sec id="s5">
<title>Author contributions</title>
<p>MG: writing-original draft, investigation; SG: review and; editing, supervision, resources. SX: investigation, visualization, review and; editing; JL: visualization, review and; editing; YW: writing-review and; editing; GZ: resources, supervision.</p>
</sec>
<sec id="s6">
<title>Funding</title>
<p>This work was supported by the National Natural Science Foundation of China (Grant Nos. 22108133, 51972180, 51572134), the Program for Scientific Research Innovation Team in Colleges and Universities of Jinan (Grant No. 2018GXRC006), and Science, Education and Industry Integration of Basic Research Projects of Qilu University of Technology (Grant No. 2022PY062).</p>
</sec>
<sec sec-type="COI-statement" id="s7">
<title>Conflict of interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="s8">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
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