Ziyue Bi, Dengfu Deng, Yuanhao Zhang, Yunfei Xie, Yi Feng, Jian Yang, Donghua Liu, Tao Liu
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{"title":"溅射高导电性掺ta的TiO2透明薄膜","authors":"Ziyue Bi, Dengfu Deng, Yuanhao Zhang, Yunfei Xie, Yi Feng, Jian Yang, Donghua Liu, Tao Liu","doi":"10.1016/j.jallcom.2025.184484","DOIUrl":null,"url":null,"abstract":"Nd or Ta doped anatase phase TiO₂ (NTO or TTO) films, prepared via pulsed laser deposition (PLD), exhibit high electrical conductivity and visible light transmittance, indicating their potential as a cheaper alternative to replace the current widely used transparent conductive oxide Sn-doped indium oxide (ITO) films. Nevertheless, these doped TiO₂ films, particularly for TTO films, prepared by an industrial-friendly sputtering method, were widely reported to have much higher resistivity. In this work, we successfully fabricated high-quality TTO thin films on SrTiO<sub>3</sub> (100) substrates using a two-step sputtering process involving low-temperature deposition followed by high-temperature annealing. The resulting TTO film achieves a low resistivity of <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mn is=\"true\">2.57</mn><mspace width=\"1em\" is=\"true\" /><mo is=\"true\">&#xD7;</mo><mspace width=\"1em\" is=\"true\" /><msup is=\"true\"><mrow is=\"true\"><mn is=\"true\">10</mn></mrow><mrow is=\"true\"><mo is=\"true\">&#x2212;</mo><mn is=\"true\">4</mn></mrow></msup><mi mathvariant=\"normal\" is=\"true\">&#x3A9;</mi><mo is=\"true\">&#x2219;</mo><mi mathvariant=\"normal\" is=\"true\">cm</mi></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.432ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -945.9 9953.8 1047.3\" width=\"23.119ex\" 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\"><use xlink:href=\"#MJMAIN-32\"></use><use x=\"500\" xlink:href=\"#MJMAIN-2E\" y=\"0\"></use><use x=\"779\" xlink:href=\"#MJMAIN-35\" y=\"0\"></use><use x=\"1279\" xlink:href=\"#MJMAIN-37\" y=\"0\"></use></g><g is=\"true\"></g><g is=\"true\" transform=\"translate(3002,0)\"><use xlink:href=\"#MJMAIN-D7\"></use></g><g is=\"true\"></g><g is=\"true\" transform=\"translate(5002,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMAIN-31\"></use><use x=\"500\" xlink:href=\"#MJMAIN-30\" y=\"0\"></use></g></g><g is=\"true\" transform=\"translate(1001,393)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-2212\"></use></g><g is=\"true\" transform=\"translate(550,0)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-34\"></use></g></g></g><g is=\"true\" transform=\"translate(7008,0)\"><use xlink:href=\"#MJMAIN-3A9\"></use></g><g is=\"true\" transform=\"translate(7953,0)\"><use xlink:href=\"#MJMAIN-2219\"></use></g><g is=\"true\" transform=\"translate(8675,0)\"><use xlink:href=\"#MJMAIN-63\"></use><use x=\"444\" xlink:href=\"#MJMAIN-6D\" y=\"0\"></use></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mn is=\"true\">2.57</mn><mspace is=\"true\" width=\"1em\"></mspace><mo is=\"true\">×</mo><mspace is=\"true\" width=\"1em\"></mspace><msup is=\"true\"><mrow is=\"true\"><mn is=\"true\">10</mn></mrow><mrow is=\"true\"><mo is=\"true\">−</mo><mn is=\"true\">4</mn></mrow></msup><mi is=\"true\" mathvariant=\"normal\">Ω</mi><mo is=\"true\">∙</mo><mi is=\"true\" mathvariant=\"normal\">cm</mi></math></span></span><script type=\"math/mml\"><math><mn is=\"true\">2.57</mn><mspace width=\"1em\" is=\"true\"></mspace><mo is=\"true\">×</mo><mspace width=\"1em\" is=\"true\"></mspace><msup is=\"true\"><mrow is=\"true\"><mn is=\"true\">10</mn></mrow><mrow is=\"true\"><mo is=\"true\">−</mo><mn is=\"true\">4</mn></mrow></msup><mi mathvariant=\"normal\" is=\"true\">Ω</mi><mo is=\"true\">∙</mo><mi mathvariant=\"normal\" is=\"true\">cm</mi></math></script></span> and a visible light transmittance of approximately 80%. This resistivity is substantially lower than previously reported sputtered TTO films and comparable to PLD-grown TTO and NTO films. Our findings demonstrate the feasibility of producing high-quality TTO films via sputtering, paving the way for their applications in high-efficiency optoelectronic devices.","PeriodicalId":344,"journal":{"name":"Journal of Alloys and Compounds","volume":"88 1","pages":""},"PeriodicalIF":6.3000,"publicationDate":"2025-10-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Sputtered highly conductive Ta-doped TiO2 transparent films\",\"authors\":\"Ziyue Bi, Dengfu Deng, Yuanhao Zhang, Yunfei Xie, Yi Feng, Jian Yang, Donghua Liu, Tao Liu\",\"doi\":\"10.1016/j.jallcom.2025.184484\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Nd or Ta doped anatase phase TiO₂ (NTO or TTO) films, prepared via pulsed laser deposition (PLD), exhibit high electrical conductivity and visible light transmittance, indicating their potential as a cheaper alternative to replace the current widely used transparent conductive oxide Sn-doped indium oxide (ITO) films. Nevertheless, these doped TiO₂ films, particularly for TTO films, prepared by an industrial-friendly sputtering method, were widely reported to have much higher resistivity. In this work, we successfully fabricated high-quality TTO thin films on SrTiO<sub>3</sub> (100) substrates using a two-step sputtering process involving low-temperature deposition followed by high-temperature annealing. 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This resistivity is substantially lower than previously reported sputtered TTO films and comparable to PLD-grown TTO and NTO films. Our findings demonstrate the feasibility of producing high-quality TTO films via sputtering, paving the way for their applications in high-efficiency optoelectronic devices.\",\"PeriodicalId\":344,\"journal\":{\"name\":\"Journal of Alloys and Compounds\",\"volume\":\"88 1\",\"pages\":\"\"},\"PeriodicalIF\":6.3000,\"publicationDate\":\"2025-10-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Alloys and Compounds\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://doi.org/10.1016/j.jallcom.2025.184484\",\"RegionNum\":2,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"CHEMISTRY, PHYSICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Alloys and Compounds","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1016/j.jallcom.2025.184484","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
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