过渡金属原子掺杂和空位调制协同增强β-NiOOH电催化析氧反应性能

IF 5.6 3区 材料科学 Q1 ELECTROCHEMISTRY
Chenghuan Zhong, Daijian Li, Shimao Xie, Pengcheng Yang, Jiao Teng, Yeyun Kang, Jianfeng Tang, Hua Lin, Chunmei Li
{"title":"过渡金属原子掺杂和空位调制协同增强β-NiOOH电催化析氧反应性能","authors":"Chenghuan Zhong, Daijian Li, Shimao Xie, Pengcheng Yang, Jiao Teng, Yeyun Kang, Jianfeng Tang, Hua Lin, Chunmei Li","doi":"10.1016/j.electacta.2025.147485","DOIUrl":null,"url":null,"abstract":"Layered <em>β</em>-NiOOH exhibits potential as a non-precious electrocatalyst for the oxygen evolution reaction (OER) owing to its tunable electronic structure through doping and defect modulating. However, the mechanistic relationship between the potential-determining step (PDS) energy barrier and the demand for modulating the electronic structure of the active center remains unresolved. This work systematically investigates the effects of compositional tuning (Cr, Mn, Fe, Co, Cu, Zn, Rh), vacancy modulation (H, O, OH), and their synergistic effect on the OER properties of <em>β</em>-NiOOH using density-functional theory calculations. Results reveal that <em>β</em>-NiOOH achieves superior OER performance through the lattice oxygen mechanism with OH as active sites, where the PDS (*O→*OOH, 0.98 V) suggests weak OHˉ adsorption and an electron-rich active center. Notably, Cu-doping combined with H-vacancy synergistically reduces the overpotential to 0.53 V. This enhancement is attributed to the co-regulation of dopant-vacancy. The d band center moved away from the Fermi level, doping-induced spin polarization promoting d-p hybridization, and increased Bader charge of *OOH from 0.67 e (<em>β</em>-NiOOH) to 1.29 e (Cu<sub>IV</sub>-NiOOH-V<sub>H-3</sub>), collectively facilitating electron escape from the active site, thereby enhancing OHˉ adsorption and lowering energy barriers. Additionally, the descriptor (<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mrow is=\"true\"&gt;&lt;mi is=\"true\"&gt;&amp;#x3C8;&lt;/mi&gt;&lt;mo linebreak=\"goodbreak\" is=\"true\"&gt;=&lt;/mo&gt;&lt;mrow is=\"true\"&gt;&lt;mrow is=\"true\"&gt;&lt;mo is=\"true\"&gt;(&lt;/mo&gt;&lt;mstyle mathvariant=\"normal\" is=\"true\"&gt;&lt;mi is=\"true\"&gt;&amp;#x394;&lt;/mi&gt;&lt;/mstyle&gt;&lt;msubsup is=\"true\"&gt;&lt;mi is=\"true\"&gt;V&lt;/mi&gt;&lt;mrow is=\"true\"&gt;&lt;mi is=\"true\"&gt;T&lt;/mi&gt;&lt;mi is=\"true\"&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;mn is=\"true\"&gt;3&lt;/mn&gt;&lt;/msubsup&gt;&lt;mo linebreak=\"badbreak\" is=\"true\"&gt;+&lt;/mo&gt;&lt;mstyle mathvariant=\"normal\" is=\"true\"&gt;&lt;mi is=\"true\"&gt;&amp;#x394;&lt;/mi&gt;&lt;/mstyle&gt;&lt;msub is=\"true\"&gt;&lt;mi is=\"true\"&gt;I&lt;/mi&gt;&lt;mn is=\"true\"&gt;1&lt;/mn&gt;&lt;/msub&gt;&lt;mo is=\"true\"&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo linebreak=\"badbreak\" is=\"true\"&gt;/&lt;/mo&gt;&lt;mrow is=\"true\"&gt;&lt;mstyle mathvariant=\"normal\" is=\"true\"&gt;&lt;mi is=\"true\"&gt;&amp;#x394;&lt;/mi&gt;&lt;/mstyle&gt;&lt;mi is=\"true\"&gt;&amp;#x3C7;&lt;/mi&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"3.24ex\" role=\"img\" style=\"vertical-align: -1.043ex;\" viewbox=\"0 -945.9 10739.3 1395\" width=\"24.943ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-3C8\"></use></g><g is=\"true\" transform=\"translate(929,0)\"><use xlink:href=\"#MJMAIN-3D\"></use></g><g is=\"true\" transform=\"translate(1985,0)\"><g is=\"true\"><use is=\"true\" xlink:href=\"#MJSZ1-28\"></use><g is=\"true\" transform=\"translate(458,0)\"><g is=\"true\"><use xlink:href=\"#MJMAIN-394\"></use></g></g><g is=\"true\" transform=\"translate(1292,0)\"><g is=\"true\"><use xlink:href=\"#MJMATHI-56\"></use></g><g is=\"true\" transform=\"translate(825,360)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-33\"></use></g><g is=\"true\" transform=\"translate(583,-320)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMATHI-54\"></use></g><g is=\"true\" transform=\"translate(498,0)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMATHI-4D\"></use></g></g></g><g is=\"true\" transform=\"translate(3439,0)\"><use xlink:href=\"#MJMAIN-2B\"></use></g><g is=\"true\" transform=\"translate(4440,0)\"><g is=\"true\"><use xlink:href=\"#MJMAIN-394\"></use></g></g><g is=\"true\" transform=\"translate(5273,0)\"><g is=\"true\"><use xlink:href=\"#MJMATHI-49\"></use></g><g is=\"true\" transform=\"translate(440,-150)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-31\"></use></g></g><use is=\"true\" x=\"6168\" xlink:href=\"#MJSZ1-29\" y=\"-1\"></use></g><g is=\"true\" transform=\"translate(6793,0)\"><use xlink:href=\"#MJMAIN-2F\"></use></g><g is=\"true\" transform=\"translate(7293,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMAIN-394\"></use></g></g><g is=\"true\" transform=\"translate(833,0)\"><use xlink:href=\"#MJMATHI-3C7\"></use></g></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mi is=\"true\">ψ</mi><mo is=\"true\" linebreak=\"goodbreak\">=</mo><mrow is=\"true\"><mrow is=\"true\"><mo is=\"true\">(</mo><mstyle is=\"true\" mathvariant=\"normal\"><mi is=\"true\">Δ</mi></mstyle><msubsup is=\"true\"><mi is=\"true\">V</mi><mrow is=\"true\"><mi is=\"true\">T</mi><mi is=\"true\">M</mi></mrow><mn is=\"true\">3</mn></msubsup><mo is=\"true\" linebreak=\"badbreak\">+</mo><mstyle is=\"true\" mathvariant=\"normal\"><mi is=\"true\">Δ</mi></mstyle><msub is=\"true\"><mi is=\"true\">I</mi><mn is=\"true\">1</mn></msub><mo is=\"true\">)</mo></mrow><mo is=\"true\" linebreak=\"badbreak\">/</mo><mrow is=\"true\"><mstyle is=\"true\" mathvariant=\"normal\"><mi is=\"true\">Δ</mi></mstyle><mi is=\"true\">χ</mi></mrow></mrow></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">ψ</mi><mo linebreak=\"goodbreak\" is=\"true\">=</mo><mrow is=\"true\"><mrow is=\"true\"><mo is=\"true\">(</mo><mstyle mathvariant=\"normal\" is=\"true\"><mi is=\"true\">Δ</mi></mstyle><msubsup is=\"true\"><mi is=\"true\">V</mi><mrow is=\"true\"><mi is=\"true\">T</mi><mi is=\"true\">M</mi></mrow><mn is=\"true\">3</mn></msubsup><mo linebreak=\"badbreak\" is=\"true\">+</mo><mstyle mathvariant=\"normal\" is=\"true\"><mi is=\"true\">Δ</mi></mstyle><msub is=\"true\"><mi is=\"true\">I</mi><mn is=\"true\">1</mn></msub><mo is=\"true\">)</mo></mrow><mo linebreak=\"badbreak\" is=\"true\">/</mo><mrow is=\"true\"><mstyle mathvariant=\"normal\" is=\"true\"><mi is=\"true\">Δ</mi></mstyle><mi is=\"true\">χ</mi></mrow></mrow></mrow></math></script></span>) for the compositional modulation of <em>β</em>-NiOOH was established, exhibiting strong correlations with valence electron count difference (Δ<em>V<sub>TM</sub></em>), first ionization energy difference (Δ<em>I</em><sub>1</sub>), and electronegativity difference (Δ<em>χ</em>) between dopants and Ni. Fitting result demonstrates a significant linear relationship between descriptor and OER overpotential variation (Δ<em>η</em>, <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mrow is=\"true\"&gt;&lt;mstyle mathvariant=\"normal\" is=\"true\"&gt;&lt;mi is=\"true\"&gt;&amp;#x394;&lt;/mi&gt;&lt;/mstyle&gt;&lt;mi is=\"true\"&gt;&amp;#x3B7;&lt;/mi&gt;&lt;mo linebreak=\"goodbreak\" is=\"true\"&gt;=&lt;/mo&gt;&lt;mo is=\"true\"&gt;&amp;#x2212;&lt;/mo&gt;&lt;mn is=\"true\"&gt;1.20&lt;/mn&gt;&lt;mi is=\"true\"&gt;&amp;#x3C8;&lt;/mi&gt;&lt;mo linebreak=\"goodbreak\" is=\"true\"&gt;+&lt;/mo&gt;&lt;mn is=\"true\"&gt;0.24&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.548ex\" role=\"img\" style=\"vertical-align: -0.697ex;\" viewbox=\"0 -796.9 8884 1096.9\" width=\"20.634ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMAIN-394\"></use></g></g><g is=\"true\" transform=\"translate(833,0)\"><use xlink:href=\"#MJMATHI-3B7\"></use></g><g is=\"true\" transform=\"translate(1614,0)\"><use xlink:href=\"#MJMAIN-3D\"></use></g><g is=\"true\" transform=\"translate(2671,0)\"><use xlink:href=\"#MJMAIN-2212\"></use></g><g is=\"true\" transform=\"translate(3449,0)\"><use xlink:href=\"#MJMAIN-31\"></use><use x=\"500\" xlink:href=\"#MJMAIN-2E\" y=\"0\"></use><use x=\"779\" xlink:href=\"#MJMAIN-32\" y=\"0\"></use><use x=\"1279\" xlink:href=\"#MJMAIN-30\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(5229,0)\"><use xlink:href=\"#MJMATHI-3C8\"></use></g><g is=\"true\" transform=\"translate(6103,0)\"><use xlink:href=\"#MJMAIN-2B\"></use></g><g is=\"true\" transform=\"translate(7104,0)\"><use xlink:href=\"#MJMAIN-30\"></use><use x=\"500\" xlink:href=\"#MJMAIN-2E\" y=\"0\"></use><use x=\"779\" xlink:href=\"#MJMAIN-32\" y=\"0\"></use><use x=\"1279\" xlink:href=\"#MJMAIN-34\" y=\"0\"></use></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mstyle is=\"true\" mathvariant=\"normal\"><mi is=\"true\">Δ</mi></mstyle><mi is=\"true\">η</mi><mo is=\"true\" linebreak=\"goodbreak\">=</mo><mo is=\"true\">−</mo><mn is=\"true\">1.20</mn><mi is=\"true\">ψ</mi><mo is=\"true\" linebreak=\"goodbreak\">+</mo><mn is=\"true\">0.24</mn></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mstyle mathvariant=\"normal\" is=\"true\"><mi is=\"true\">Δ</mi></mstyle><mi is=\"true\">η</mi><mo linebreak=\"goodbreak\" is=\"true\">=</mo><mo is=\"true\">−</mo><mn is=\"true\">1.20</mn><mi is=\"true\">ψ</mi><mo linebreak=\"goodbreak\" is=\"true\">+</mo><mn is=\"true\">0.24</mn></mrow></math></script></span>, R<sup>2</sup> = 0.92). This work offers practical and theoretical guidance for the development of high-performance OER electrocatalysts.","PeriodicalId":305,"journal":{"name":"Electrochimica Acta","volume":"33 1","pages":""},"PeriodicalIF":5.6000,"publicationDate":"2025-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Synergistic Enhancement of β-NiOOH Electrocatalytic Oxygen Evolution Reaction Performance through Transition Metal Atom Doping and Vacancy Modulating\",\"authors\":\"Chenghuan Zhong, Daijian Li, Shimao Xie, Pengcheng Yang, Jiao Teng, Yeyun Kang, Jianfeng Tang, Hua Lin, Chunmei Li\",\"doi\":\"10.1016/j.electacta.2025.147485\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Layered <em>β</em>-NiOOH exhibits potential as a non-precious electrocatalyst for the oxygen evolution reaction (OER) owing to its tunable electronic structure through doping and defect modulating. However, the mechanistic relationship between the potential-determining step (PDS) energy barrier and the demand for modulating the electronic structure of the active center remains unresolved. This work systematically investigates the effects of compositional tuning (Cr, Mn, Fe, Co, Cu, Zn, Rh), vacancy modulation (H, O, OH), and their synergistic effect on the OER properties of <em>β</em>-NiOOH using density-functional theory calculations. Results reveal that <em>β</em>-NiOOH achieves superior OER performance through the lattice oxygen mechanism with OH as active sites, where the PDS (*O→*OOH, 0.98 V) suggests weak OHˉ adsorption and an electron-rich active center. Notably, Cu-doping combined with H-vacancy synergistically reduces the overpotential to 0.53 V. This enhancement is attributed to the co-regulation of dopant-vacancy. The d band center moved away from the Fermi level, doping-induced spin polarization promoting d-p hybridization, and increased Bader charge of *OOH from 0.67 e (<em>β</em>-NiOOH) to 1.29 e (Cu<sub>IV</sub>-NiOOH-V<sub>H-3</sub>), collectively facilitating electron escape from the active site, thereby enhancing OHˉ adsorption and lowering energy barriers. Additionally, the descriptor (<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;&amp;#x3C8;&lt;/mi&gt;&lt;mo linebreak=\\\"goodbreak\\\" is=\\\"true\\\"&gt;=&lt;/mo&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mo is=\\\"true\\\"&gt;(&lt;/mo&gt;&lt;mstyle mathvariant=\\\"normal\\\" is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;&amp;#x394;&lt;/mi&gt;&lt;/mstyle&gt;&lt;msubsup is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;V&lt;/mi&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;T&lt;/mi&gt;&lt;mi is=\\\"true\\\"&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;mn is=\\\"true\\\"&gt;3&lt;/mn&gt;&lt;/msubsup&gt;&lt;mo linebreak=\\\"badbreak\\\" is=\\\"true\\\"&gt;+&lt;/mo&gt;&lt;mstyle mathvariant=\\\"normal\\\" is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;&amp;#x394;&lt;/mi&gt;&lt;/mstyle&gt;&lt;msub is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;I&lt;/mi&gt;&lt;mn is=\\\"true\\\"&gt;1&lt;/mn&gt;&lt;/msub&gt;&lt;mo is=\\\"true\\\"&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo linebreak=\\\"badbreak\\\" is=\\\"true\\\"&gt;/&lt;/mo&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mstyle mathvariant=\\\"normal\\\" is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;&amp;#x394;&lt;/mi&gt;&lt;/mstyle&gt;&lt;mi is=\\\"true\\\"&gt;&amp;#x3C7;&lt;/mi&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"3.24ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -1.043ex;\\\" viewbox=\\\"0 -945.9 10739.3 1395\\\" width=\\\"24.943ex\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g fill=\\\"currentColor\\\" stroke=\\\"currentColor\\\" stroke-width=\\\"0\\\" transform=\\\"matrix(1 0 0 -1 0 0)\\\"><g is=\\\"true\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-3C8\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(929,0)\\\"><use xlink:href=\\\"#MJMAIN-3D\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(1985,0)\\\"><g is=\\\"true\\\"><use is=\\\"true\\\" xlink:href=\\\"#MJSZ1-28\\\"></use><g is=\\\"true\\\" transform=\\\"translate(458,0)\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMAIN-394\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(1292,0)\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-56\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(825,360)\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-33\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(583,-320)\\\"><g is=\\\"true\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMATHI-54\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(498,0)\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMATHI-4D\\\"></use></g></g></g><g is=\\\"true\\\" transform=\\\"translate(3439,0)\\\"><use xlink:href=\\\"#MJMAIN-2B\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(4440,0)\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMAIN-394\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(5273,0)\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-49\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(440,-150)\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-31\\\"></use></g></g><use is=\\\"true\\\" x=\\\"6168\\\" xlink:href=\\\"#MJSZ1-29\\\" y=\\\"-1\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(6793,0)\\\"><use xlink:href=\\\"#MJMAIN-2F\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(7293,0)\\\"><g is=\\\"true\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMAIN-394\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(833,0)\\\"><use xlink:href=\\\"#MJMATHI-3C7\\\"></use></g></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">ψ</mi><mo is=\\\"true\\\" linebreak=\\\"goodbreak\\\">=</mo><mrow is=\\\"true\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">(</mo><mstyle is=\\\"true\\\" mathvariant=\\\"normal\\\"><mi is=\\\"true\\\">Δ</mi></mstyle><msubsup is=\\\"true\\\"><mi is=\\\"true\\\">V</mi><mrow is=\\\"true\\\"><mi is=\\\"true\\\">T</mi><mi is=\\\"true\\\">M</mi></mrow><mn is=\\\"true\\\">3</mn></msubsup><mo is=\\\"true\\\" linebreak=\\\"badbreak\\\">+</mo><mstyle is=\\\"true\\\" mathvariant=\\\"normal\\\"><mi is=\\\"true\\\">Δ</mi></mstyle><msub is=\\\"true\\\"><mi is=\\\"true\\\">I</mi><mn is=\\\"true\\\">1</mn></msub><mo is=\\\"true\\\">)</mo></mrow><mo is=\\\"true\\\" linebreak=\\\"badbreak\\\">/</mo><mrow is=\\\"true\\\"><mstyle is=\\\"true\\\" mathvariant=\\\"normal\\\"><mi is=\\\"true\\\">Δ</mi></mstyle><mi is=\\\"true\\\">χ</mi></mrow></mrow></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mi is=\\\"true\\\">ψ</mi><mo linebreak=\\\"goodbreak\\\" is=\\\"true\\\">=</mo><mrow is=\\\"true\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">(</mo><mstyle mathvariant=\\\"normal\\\" is=\\\"true\\\"><mi is=\\\"true\\\">Δ</mi></mstyle><msubsup is=\\\"true\\\"><mi is=\\\"true\\\">V</mi><mrow is=\\\"true\\\"><mi is=\\\"true\\\">T</mi><mi is=\\\"true\\\">M</mi></mrow><mn is=\\\"true\\\">3</mn></msubsup><mo linebreak=\\\"badbreak\\\" is=\\\"true\\\">+</mo><mstyle mathvariant=\\\"normal\\\" is=\\\"true\\\"><mi is=\\\"true\\\">Δ</mi></mstyle><msub is=\\\"true\\\"><mi is=\\\"true\\\">I</mi><mn is=\\\"true\\\">1</mn></msub><mo is=\\\"true\\\">)</mo></mrow><mo linebreak=\\\"badbreak\\\" is=\\\"true\\\">/</mo><mrow is=\\\"true\\\"><mstyle mathvariant=\\\"normal\\\" is=\\\"true\\\"><mi is=\\\"true\\\">Δ</mi></mstyle><mi is=\\\"true\\\">χ</mi></mrow></mrow></mrow></math></script></span>) for the compositional modulation of <em>β</em>-NiOOH was established, exhibiting strong correlations with valence electron count difference (Δ<em>V<sub>TM</sub></em>), first ionization energy difference (Δ<em>I</em><sub>1</sub>), and electronegativity difference (Δ<em>χ</em>) between dopants and Ni. Fitting result demonstrates a significant linear relationship between descriptor and OER overpotential variation (Δ<em>η</em>, <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mstyle mathvariant=\\\"normal\\\" is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;&amp;#x394;&lt;/mi&gt;&lt;/mstyle&gt;&lt;mi is=\\\"true\\\"&gt;&amp;#x3B7;&lt;/mi&gt;&lt;mo linebreak=\\\"goodbreak\\\" is=\\\"true\\\"&gt;=&lt;/mo&gt;&lt;mo is=\\\"true\\\"&gt;&amp;#x2212;&lt;/mo&gt;&lt;mn is=\\\"true\\\"&gt;1.20&lt;/mn&gt;&lt;mi is=\\\"true\\\"&gt;&amp;#x3C8;&lt;/mi&gt;&lt;mo linebreak=\\\"goodbreak\\\" is=\\\"true\\\"&gt;+&lt;/mo&gt;&lt;mn is=\\\"true\\\"&gt;0.24&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.548ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.697ex;\\\" viewbox=\\\"0 -796.9 8884 1096.9\\\" width=\\\"20.634ex\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g fill=\\\"currentColor\\\" stroke=\\\"currentColor\\\" stroke-width=\\\"0\\\" transform=\\\"matrix(1 0 0 -1 0 0)\\\"><g is=\\\"true\\\"><g is=\\\"true\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMAIN-394\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(833,0)\\\"><use xlink:href=\\\"#MJMATHI-3B7\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(1614,0)\\\"><use xlink:href=\\\"#MJMAIN-3D\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(2671,0)\\\"><use xlink:href=\\\"#MJMAIN-2212\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(3449,0)\\\"><use xlink:href=\\\"#MJMAIN-31\\\"></use><use x=\\\"500\\\" xlink:href=\\\"#MJMAIN-2E\\\" y=\\\"0\\\"></use><use x=\\\"779\\\" xlink:href=\\\"#MJMAIN-32\\\" y=\\\"0\\\"></use><use x=\\\"1279\\\" xlink:href=\\\"#MJMAIN-30\\\" y=\\\"0\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(5229,0)\\\"><use xlink:href=\\\"#MJMATHI-3C8\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(6103,0)\\\"><use xlink:href=\\\"#MJMAIN-2B\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(7104,0)\\\"><use xlink:href=\\\"#MJMAIN-30\\\"></use><use x=\\\"500\\\" xlink:href=\\\"#MJMAIN-2E\\\" y=\\\"0\\\"></use><use x=\\\"779\\\" xlink:href=\\\"#MJMAIN-32\\\" y=\\\"0\\\"></use><use x=\\\"1279\\\" xlink:href=\\\"#MJMAIN-34\\\" y=\\\"0\\\"></use></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mstyle is=\\\"true\\\" mathvariant=\\\"normal\\\"><mi is=\\\"true\\\">Δ</mi></mstyle><mi is=\\\"true\\\">η</mi><mo is=\\\"true\\\" linebreak=\\\"goodbreak\\\">=</mo><mo is=\\\"true\\\">−</mo><mn is=\\\"true\\\">1.20</mn><mi is=\\\"true\\\">ψ</mi><mo is=\\\"true\\\" linebreak=\\\"goodbreak\\\">+</mo><mn is=\\\"true\\\">0.24</mn></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mstyle mathvariant=\\\"normal\\\" is=\\\"true\\\"><mi is=\\\"true\\\">Δ</mi></mstyle><mi is=\\\"true\\\">η</mi><mo linebreak=\\\"goodbreak\\\" is=\\\"true\\\">=</mo><mo is=\\\"true\\\">−</mo><mn is=\\\"true\\\">1.20</mn><mi is=\\\"true\\\">ψ</mi><mo linebreak=\\\"goodbreak\\\" is=\\\"true\\\">+</mo><mn is=\\\"true\\\">0.24</mn></mrow></math></script></span>, R<sup>2</sup> = 0.92). 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引用次数: 0

摘要

层状β-NiOOH具有通过掺杂和缺陷调制可调谐的电子结构,具有作为析氧反应(OER)的非贵重电催化剂的潜力。然而,势决定步长(PDS)能垒与调制活性中心电子结构的需求之间的机制关系仍未得到解决。本研究利用密度泛函理论计算系统地研究了成分调谐(Cr, Mn, Fe, Co, Cu, Zn, Rh)和空位调制(H, O, OH)的影响,以及它们对β-NiOOH OER特性的协同效应。结果表明,β-NiOOH通过以OH为活性位点的点阵氧机制获得了优异的OER性能,其中PDS (*O→*OOH, 0.98 V)表明弱OH - h的吸附和富电子的活性中心。值得注意的是,cu掺杂与h空位协同作用将过电位降低到0.53 V。这种增强归因于掺杂剂空位的共同调节。d带中心远离费米能级,掺杂诱导的自旋极化促进了d-p杂化,使*OOH的Bader电荷从0.67 e (β-NiOOH)增加到1.29 e (CuIV-NiOOH-VH-3),共同促进了电子从活性位点逃逸,从而增强了OH- h的吸附,降低了能垒。此外,描述符(ψ=(ΔVTM3 +ΔI1) /Δχψ=(ΔVTM3 +ΔI1) /Δχ)成分调制的β-NiOOH成立,表现出强烈的相关性与价电子数差异(ΔVTM),第一电离能差异(ΔI1)和电负性差异(Δχ)掺杂物和倪之间。拟合结果表明,描述子与OER过电位变化之间存在显著的线性关系(Δη, Δη= - 1.20ψ+0.24Δη= - 1.20ψ+0.24, R2 = 0.92)。本研究为高性能OER电催化剂的开发提供了理论和实践指导。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Synergistic Enhancement of β-NiOOH Electrocatalytic Oxygen Evolution Reaction Performance through Transition Metal Atom Doping and Vacancy Modulating

Synergistic Enhancement of β-NiOOH Electrocatalytic Oxygen Evolution Reaction Performance through Transition Metal Atom Doping and Vacancy Modulating
Layered β-NiOOH exhibits potential as a non-precious electrocatalyst for the oxygen evolution reaction (OER) owing to its tunable electronic structure through doping and defect modulating. However, the mechanistic relationship between the potential-determining step (PDS) energy barrier and the demand for modulating the electronic structure of the active center remains unresolved. This work systematically investigates the effects of compositional tuning (Cr, Mn, Fe, Co, Cu, Zn, Rh), vacancy modulation (H, O, OH), and their synergistic effect on the OER properties of β-NiOOH using density-functional theory calculations. Results reveal that β-NiOOH achieves superior OER performance through the lattice oxygen mechanism with OH as active sites, where the PDS (*O→*OOH, 0.98 V) suggests weak OHˉ adsorption and an electron-rich active center. Notably, Cu-doping combined with H-vacancy synergistically reduces the overpotential to 0.53 V. This enhancement is attributed to the co-regulation of dopant-vacancy. The d band center moved away from the Fermi level, doping-induced spin polarization promoting d-p hybridization, and increased Bader charge of *OOH from 0.67 e (β-NiOOH) to 1.29 e (CuIV-NiOOH-VH-3), collectively facilitating electron escape from the active site, thereby enhancing OHˉ adsorption and lowering energy barriers. Additionally, the descriptor (ψ=(ΔVTM3+ΔI1)/Δχ) for the compositional modulation of β-NiOOH was established, exhibiting strong correlations with valence electron count difference (ΔVTM), first ionization energy difference (ΔI1), and electronegativity difference (Δχ) between dopants and Ni. Fitting result demonstrates a significant linear relationship between descriptor and OER overpotential variation (Δη, Δη=1.20ψ+0.24, R2 = 0.92). This work offers practical and theoretical guidance for the development of high-performance OER electrocatalysts.
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来源期刊
Electrochimica Acta
Electrochimica Acta 工程技术-电化学
CiteScore
11.30
自引率
6.10%
发文量
1634
审稿时长
41 days
期刊介绍: Electrochimica Acta is an international journal. It is intended for the publication of both original work and reviews in the field of electrochemistry. Electrochemistry should be interpreted to mean any of the research fields covered by the Divisions of the International Society of Electrochemistry listed below, as well as emerging scientific domains covered by ISE New Topics Committee.
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